Mesoporous oxides as efficient catalysts for the
electrocatalytic oxygen evolution reaction (OER)
vorgelegt von
Diplom-Chemiker Michael Bernicke
geb. in Berlin
Von der Fakultät II - Mathematik und Naturwissenschaften
der Technischen Universität Berlin
zur Erlangung des akademischen Grades
Doktor der Naturwissenschaften
Dr. rer. nat.
genehmigte Dissertation
Promotionsausschuss:
Vorsitzender: Prof. Dr. Thomas Friedrich
Gutachter: Dr.-Ing. Ralph Krähnert
Gutachter: Prof. Dr. Peter Strasser
Gutachter: Prof. Dr. Michael Bron
Tag der wissenschaftlichen Aussprache: 7. September 2016
Berlin 2016
Wir sind gleichsam Zwerge, die auf den Schultern von Riesen sitzen, um mehr und
Entfernteres als diese sehen zu können - freilich nicht dank eigener scharfer Sehkraft oder
Körpergröße, sondern weil die Größe der Riesen uns zu Hilfe kommt und uns emporhebt.
- Bernhard von Chartres
Danksagung
Ich danke Dr.-Ing. Ralph Krähnert für die Aufnahme in den Arbeitskreis und die Möglichkeit
der Promotion. Durch anregende und strukturierte wissenschaftliche Diskussionen war
immer ein effizientes Arbeiten im Laufe meiner Promotion möglich. Für die unzähligen
Ratschläge und die fruchtbare Zusammenarbeit möchte ich mich bedanken.
Bei Herrn Professor Thomas Friedrich bedanke ich mich für die bereitwillige Übernahme der
Funktion des Vorsitzenden und bei den Herren Professoren Peter Strasser und Michael Bron
bedanke ich mich für die Erstellung des Gutachtens.
Mein weiterer Dank gilt Erik Ortel für die freundliche Einweisung in die Künste eines
Doktoranden. Bei Tobias Reier, Arno Bergmann und Nadine Menzel möchte ich mich für die
vielen Ratschläge zu Beginn und während meiner Promotion bedanken. Mein besonderer
Dank gilt hierbei Tobias Reier, der unzählige Stunden damit verbracht hat, mich in die
Geheimnisse der Elektrokatalyse einzuweihen. Des Weiteren bedanke ich mich bei Andreas
Lippitz für XPS- und Eicke Gericke für SAXS-Messungen. Besonders möchte ich Kornelia
Weh für zahlreiche ICP-Messungen danken. Bei Denis Bernsmeier bedanke ich mich für
bereitwilliges Messen von SAXS und BET. Björn Eckhardt und Katrin Schulz danke ich für
viele XRD-Messungen. Ich danke Jorge Araujo für DEMS-Messungen. Des Weiteren möchte
ich mich bei Erik Ortel, Benjamin Paul, Roman Schmack und allen Mitarbeitern des ZELMI
für unzählige elektronenmikroskopische Bilder bedanken. Nicolas Chaoui, Jérôme Roeser,
Nathaniel Leonard und vor allem Ebru Özer danke ich für sorgfältiges Korrekturlesen.
Bei meinen Kollegen Denis Bernsmeier, Björn Eckhardt, Roman Schmack, Katrin Schulz,
Benjamin Paul, Huan Wang und René Sachse möchte ich mich für ein angenehmes
Arbeitsklima und die gemeinsamen Abende mit viel Spaß bedanken.
Der Arbeitsgruppe von Herrn Professor Strasser danke ich für die angenehme
Arbeitsatmosphäre und die stundenlangen Freuden am Kickertisch. Besonders hervorheben
möchte ich hierbei Ebru Özer, Camillo Spöri, Hong Nhan, Tobias Reier, Vera Beermann,
Henrike Schmieß, Julian Steinberg, Malte Klingenhof, Thomas Merzdorf, Henner Heyen und
Elisabeth Hornberger.
Zu guter Letzt möchte ich mich bei meinen Eltern und meiner restlichen Familie für die
ständige Unterstützung in meinem Leben bedanken. Ihr wart immer an meiner Seite und
habt mich unterstützt, wo ihr nur konntet, dafür möchte ich euch von ganzem Herzen
danken!
Zusammenfassung
Wasserstoff ist ein wichtiger Energieträger der Zukunft und findet Verwendung in einer
Vielzahl industrieller Prozesse. Die elektrokatalytische Wasserspaltung stellt eine wichtige
Möglichkeit der Wasserstoffgewinnung dar und wird durch einen komplexen Mechanismus
an der sauerstofferzeugenden Anode limitiert. Die Erhöhung der Massenaktivität eingesetzter
Katalysatoren führt zur Verringerung der Investitionskosten von Elektrolyseuren.
Die vorliegende Doktorarbeit zeigt die Synthese mesoporöser Oxidfilme als saure oder
alkalische OER-Elektrokatalysatoren. Die Katalysatoren basieren auf unterschiedlichen
Metalloxiden, wie NiO, IrO2 und IrO2/TiO2. Die Herstellung oxidischer Filme erfolgte mittels
Tauchbeschichtung und basiert auf einer verdampfungsinduzierten Selbstanordnung eines
PEO-b-PB-b-PEO Blockcopolymers als Porentemplat und eines geeigneten
Metalloxidpräkursors sowie einer anschließenden thermischen Behandlung. Die jeweiligen
Synthesen und physikochemischen Charakterisierungen der einzelnen Verbindungen
werden im Diskussionsteil beschrieben.
Die Korrelation von Struktur und OER-Aktivität erlaubte das Ableiten von Struktur-Aktivitäts-
Beziehungen. Diese Beziehungen konnten genutzt werden, um OER-Einflussparameter zu
identifizieren. Die Verwendung verschiedener Systeme mit spezifischen Eigenschaften
erlaubte die gezielte Untersuchung der wichtigsten OER-Einflussparameter. Durch
Zusammenfassen der wichtigsten OER-Einflussparameter wurde ein mögliches OER-Model
vorgeschlagen. Das OER-Model beschreibt, bei welchen strukturellen Eigenschaften hohe
OER-Aktivitäten erwartet werden können. Zusätzlich wurde der Einfluss auf kinetische
Kenngrößen, wie etwa dem Tafelanstieg, berücksichtigt. Hohe OER-Aktivitäten und geringe
Tafelanstiege werden vor allem für Materialien mit geringer Kristallitgröße, hoher aktiver
Oberfläche, hoher Leitfähigkeit sowie bei elektrokatalytischen Messungen mit moderaten
Überspannungen (ca. η < 0.35 V) beobachtet.
Katalysatoren, welche nach dem postulierten OER-Model, hohe OER-Aktivitäten zeigen,
wurden mit kommerziellen Referenzsystemen verglichen. Es konnte gezeigt werden, dass
die in dieser Arbeit hergestellten Oxidfilme über eine 11- bis 24- fach höhere OER-Aktivität
bezogen auf die eingesetzte Masse an Iridium Metall im Vergleich zu kommerziell
verfügbaren Katalysatorpulvern verfügen.
Abstract
Hydrogen is considered an important energy carrier and feedstock for industrial applications.
The generation of hydrogen can be realised by electrocatalytic water splitting. However, the
efficiency of water electrolysers is limited by the slow kinetics of oxygen evolution reaction
(OER). An increase in mass based OER activity is mandatory for a lower capital cost of
electrolyser cells.
In this thesis, synthesis routes are presented for new mesoporous metal oxide films used as
catalytic layers for OER in alkaline or acidic media. The catalytic layers contain different
metal oxides, such as NiO, IrO2 and IrO2/TiO2. The synthesis of metal oxide coatings with
high accessible ordered mesopore structure was achieved via evaporation induced self
assembly. The synthesis succeeds by utilizing PEO-b-PB-b-PEO triblock copolymers as a
pore template, a suitable metal oxide precursor, and a final heat treatment under air. The
synthesis conditions and corresponding physicochemical characterisations are shown in the
discussion.
Correlation of structure and OER activity was used to deduce structure-activity relationships.
These relationships were then used to identify the most significant OER-controlling
parameters. All identified OER-controlling parameters were combined in order to develop an
OER-model describing which structural properties benefit OER activity the most.
Furthermore, the influence on kinetic parameters such as Tafel slope was investigated. High
OER-activities and low Tafel slopes were found for materials with low crystallinity, high
surface area, high conductivity and electrocatalytic measurements conducted at moderate
overpotentials (ca. η < 0,35 V).
In order to demonstrate the commercial relevance of the catalytic layers synthesised in this
work, their OER activity was compared with commercial reference catalysts. It was shown
that oxide layers of this work exhibit a 11 to 24 times higher iridium mass based OER activity
compared to commercial reference catalysts.
Published work
Note that parts of this thesis were already published and that reuse solely for this document
was permitted by John Wiley and Sons.
M. Bernicke, B. Eckhardt, A. Lippitz, E. Ortel, D. Bernsmeier, R. Schmack, R. Kraehnert,
ChemistrySelect 2016, 3, 1-9. http://dx.doi.org/10.1002/slct.201600110
M. Bernicke, E. Ortel, T. Reier, A. Bergmann, J. Ferreira de Araujo, P. Strasser, R.
Kraehnert, ChemSusChem 2015, 8, 1908-1915. http://dx.doi.org/10.1002/cssc.201402988
Contents
1 Motivation ........................................................................................................................... 1
2 State of the Art ................................................................................................................... 2
2.1 Electrocatalytic water splitting and electric properties .................................................. 2
2.2 Oxides with templated porosity ...................................................................................13
2.3 Synthesis routes for metal oxides ...............................................................................21
2.4 Deduced thesis aim and approaches ..........................................................................26
2.5 Thesis outline ..............................................................................................................27
3 Experimental .....................................................................................................................29
3.1 Synthesis of micelle-templated films ...........................................................................29
3.2 Analytical methods ......................................................................................................32
3.3 Electrocatalytic testing ................................................................................................35
4 Results and discussion ......................................................................................................37
4.1 Mesoporous templated NiO synthesized from Ni(NO3)2 and citric acid ........................38
4.2 Mesoporous templated IrO2 synthesized from Ir(OAc)3 ...............................................50
4.3 Mesoporous templated IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4 ........................65
4.4 Mesoporous templated IrO2/TiO2 synthesized from Ir(OAc)3 and TALH ......................78
4.5 Reference catalysts ....................................................................................................95
5 General discussion ............................................................................................................99
5.1 Influence of precursor on structure/morphology (TiO2, IrO2, IrO2/TiO2) ...................... 101
5.2 Influence of calcination temperature on morphology (TiO2, IrO2, IrO2/TiO2) ............... 104
5.3 Processes during synthesis and the resulting morphology ........................................ 107
5.4 Influence of calcination temperature on OER activity and ECSA ............................... 111
5.5 Influence of crystallinity on OER activity .................................................................... 112
5.6 Influence of electrical conductivity on OER activity .................................................... 114
5.7 Influence of layer thickness on gas removal rate ....................................................... 117
5.8 Tafel slope as a function of calcination temperature and potential ............................ 120
5.9 Investigation of Tafel slopes as a function of iridium loading and potential ................ 123
5.10 Deduced structure-activity relations ........................................................................ 124
5.11 Comparison of iridium-mass based OER activity ..................................................... 127
6 Conclusions and Outlook ................................................................................................. 130
References ......................................................................................................................... 132
Appendix ............................................................................................................................ 138
Acronyms ........................................................................................................................... 141
1
1 Motivation
Modern society consumes huge amounts of energy relying on the combustion of fossil
resources. The amount of fossil resources such as coal and oil is limited. Therefore, new
routes of energy conversion and storage have to be developed.
Molecular hydrogen (H2) has the highest mass specific energy density of all chemical fuels[1]
and thus appears to be a very attractive candidate for energy storage. The stored energy can
be regained as electrical energy in fuel cells[2] with water as a byproduct. However, depletion
of fossil resources[3] and competition with other industrial applications (e. g. Haber-Bosch-
process,[4] HCl-synthesis,[5] metal oxide reduction[6] and Fischer-Tropsch-Synthesis[7]) require
efficient and sustainable routes for hydrogen generation.
Many routes for generating molecular H2 are available, i.e. it is commonly generated by the
reaction of zinc and hydrochloric acid[8] for laboratory scale purposes. The reaction is
considered as uneconomic thus industrial generation of hydrogen relies on steam reforming[9]
and partial oxidation of methane[10] accompanied by the production of unwanted greenhouse
gases, i.e. CO2.
Several approaches for water splitting are available, such as photocatalysis,[11] thermal water
splitting[12] or water electrolysis.[13] Due to nonpolluting operation conditions and fairly high
efficiencies of 93 % (εΔH),[14] electrocatalytic water splitting is considered a promising
candidate for establishing a sustainable hydrogen economy. Clean energy economy without
indirect CO2 formation is established only when feeding the required energy for electrolysis
from renewable energy sources, such as solar or wind energy.
The efficiency and competiveness of water electrolysis is limited by a complex reaction
mechanism of the oxygen evolution reaction (OER) causing a high anodic overpotential. The
development and improvement of novel electrocatalysts is considered as the major task to
overcome these roadblocks in energy conversion.
2
2 State of the Art
The following chapter (2) introduces general aspects that are most relevant for the present
thesis. Chapter 2.1 presents principles of electrocatalytic water splitting in alkaline and acidic
electrolyte solutions. Moreover, the chapter contains literature reports of electrocatalysts
used for the oxygen evolution reaction in both media. The reported electrocatalysts usually
contain metal oxides. An increase in surface area is often used to enhance activity which can
be achieved by the introduction of porosity. Chapter 2.2 presents general synthesis concepts
for the preparation of oxides with templated porosity such as evaporation induced self
assembly (EISA). Chapter 2.3 introduces reports from literature exploiting EISA and polymer
template based synthesis routes for the preparation of different mesoporous metal oxides,
i.e. oxides of Al, Mg, Co, Zn, Ti and Ir. The presented synthesis routes are of particular
interest to achieve the specified goals in this thesis (chapter 2.4). A roadmap for the
successful realisation of the aims is presented in chapter 2.5.
2.1 Electrocatalytic water splitting and electric properties
The history of water electrolysis began in the beginning of the 19th century with the discovery
by Nicholson and Carlisle of electrocatalytic water splitting.[15] A century later more than 400
industrial water electrolysis devices were in operation. The first large water electrolysis plant
was deployed in 1939 and provided hydrogen production rates of 10 000 Nm³H2/h. The first
industrial electrolyser capable to work under pressurized conditions was developed in 1948
by Zdansky/Lonza. The development of water electrolysers was continued with the
construction of the first solid polymer electrolyte system by General Electric in 1966. In 1972
the first solid oxide water electrolysis units were introduced.
The following chapter 2.1 deduces the thermodynamic standard potential required for the
electrocatalytic water splitting (2.1.1). Advantages, disadvantages and typical OER catalysts
used for water splitting in alkaline (chapters 2.1.2 - 2.1.3) and acidic media (chapters 2.1.4 -
2.1.5) are presented. Finally, basic investigations reported in literature on structure-activity
relationships are shown for state of the art catalysts used in acidic water splitting, i.e. iridium
oxide. The presented publications underline effects on OER activity and electron transport
mechanism, i.e. layer thickness (chapter 2.1.6), calcination temperature (chapter 2.1.7) and
electrical conductivity (chapter 2.1.8).
3
2.1.1 Thermodynamic standard potential of water splitting
The net balance for electrochemical water splitting is:
H2O ½ O2 + H2 | ΔH0 = 285.8 kJ/mol
The minimal required voltage E0 that has to be applied under standard conditions (p,T =
constant) in order to carry out electrolysis of water is expressed as:
𝐸0=−∆𝐺0
𝑛 ∙ 𝐹
Wherein ΔG0 is referred to as the change in Gibbs free energy under standard conditions, F
is related to the Faraday constant (96 485 C/mol) and n expresses the number of electrons
transferred during reaction (in this case n=2).
The fundamental Gibbs-Helmholtz equation is expressed as followed:
∆𝐺0=∆𝐻0− 𝑇∆𝑆0
For water electrolysis under standard conditions the standard reaction enthalpy ΔH0 amounts
to 285.8 kJ/mol, whereas the standard molar entropies ΔS0 are found to be:
∆𝑆0(𝐻2)=130.7 𝐽
𝐾 ∙ 𝑚𝑜𝑙 ; ∆𝑆0(𝑂2)=205.1 𝐽
𝐾 ∙ 𝑚𝑜𝑙 ; ∆𝑆0(𝐻2𝑂) = 70 𝐽
𝐾 ∙ 𝑚𝑜𝑙
The total change of molar entropy for the electrolysis of water is expressed as:
∆𝑆𝑡𝑜𝑡𝑎𝑙
0=∆𝑆0(𝐻2) + 0.5 ∙ ∆𝑆0(𝑂2)− ∆𝑆0(𝐻2𝑂)
And amounts to the following value:
∆𝑆𝑡𝑜𝑡𝑎𝑙
0=(130.6 + 0.5 ∙205.1 −70)𝐽
𝐾 ∙ 𝑚𝑜𝑙 =𝟏𝟔𝟑.𝟏𝟓 𝑱
𝑲 ∙ 𝒎𝒐𝒍
Inserting ΔS0 and ΔH0 in the Gibbs-Helmholtz equation allows the determination of Gibbs free
energy ΔG0 under standard conditions (298 K, 1 bar):
∆𝐺0=∆𝐻0− 𝑇∆𝑆0=285.8 𝑘𝐽
𝑚𝑜𝑙 −298 𝐾 ∙ 163.15 𝐽
𝐾 ∙ 𝑚𝑜𝑙 =𝟐𝟑𝟔.𝟖𝟖 𝒌𝑱
𝒎𝒐𝒍
4
Moreover the minimum required potential for the beginning of water electrolysis in an open
cell can be determined:
𝐸𝑐𝑒𝑙𝑙
0=−∆𝐺0
𝑛 ∙ 𝐹 =
−𝟐𝟑𝟔.𝟖𝟖 𝒌𝑱
𝒎𝒐𝒍
2∙96485 𝐶
𝑚𝑜𝑙
=−1.23 𝐽
𝐶=−𝟏.𝟐𝟑 𝑽
The negative value indicates that the reaction does not occur spontaneously thus requiring
energy to proceed. In conclusion, the determined voltage as high as 1.23 V is considered as
the thermodynamic minimum potential required for water electrolysis under standard
conditions (25 °C, 1 bar).
Water splitting usually is conducted in either acidic or alkaline media. The advantages and
disadvantages for electrolysers operating in various media are discussed in chapters 2.1.2 -
2.1.5.
2.1.2 General aspects of alkaline water splitting
Alkaline water splitting is characterized by two electrodes immersed in a solution typically
containing 20 % - 30 % KOH. Both electrodes are separated from each other by a diaphragm
ensuring physical segregation of evolving O2 and H2 at the anode and cathode, respectively.
The separation of both gases is necessary for the sake of safety and efficiency. The utilized
diaphragm is permeable for hydroxide and water molecules in order to provide transport of
reactants between both reaction chambers.[13]
Figure 1: Schematic illustration of an alkaline electro-catalytic water splitting cell. Anode and Cathode are
separated by a diaphragm to inhibit cross diffusion.
Anode
OER catalyst
(Ni/Co/Fe)
Cathode
HER catalyst
(Ni)
Diaphragm
½ O
2
H
2
OH
-
H
2
O
5
The half-cell reactions for water splitting in alkaline media are:
anode: 4 OH- → 2 H2O + O2 + 4 e-
cathode: 4 H2O + 4 e- → 2 H2 + 4 OH-
overall: 2 H2O → 2 H2 + O2
A closer look at alkaline electro-catalytic water splitting cells reveals several disadvantages.
First, the diaphragm does not fully separate the evolving gases. As a result, evolving O2
diffuses from the anode to the cathode and H2 diffuses from the cathode to the anode. This
cross-diffusion leads to decreased efficiency by the reduction of enriched O2 at the cathode
and can be potentially dangerous due to the formation of a hazardous mixture of O2 and H2 in
the anode chamber. A shutdown and subsequent purge of the chamber with inert gas is
required in order to prevent damage.[13]
The cross diffusion rate is independent of current density. The contamination of both cell
chambers caused by crosss diffusion thus proceeds rather quickly at low production rates
and low current densities. As a result, hazardous working conditions are reached fast and
should be avoided by using high production rates in order to flush the contaminants from the
system.[13]
Many other problems are associated with the use of liquid electrolyte and diaphragms.
Notably, high ohmic losses occur throughout the liquid electrolyte and diaphragm which limits
the maximum achievable current density. Moreover, operation at high pressures is not
possible which results in a clunky stack design.[13]
2.1.3 OER catalysts used in alkaline media
Catalysts used for oxygen evolution in alkaline media are typically based on the oxides,
oxyhydroxides or hydroxides of metals such as CoOx,[16-19] CoFeOx,[16, 20-21] NiOx,[22-27]
NiCeOx,[22] NiCoOx,[28] NiCuOx,[28] NiFeOx,[16, 29-33] NiLaOx,[22] MnOx,[34-35] MnCoOx.[36]
Several reports in the literature show investigations on the electrocatalytic activity of nickel
based water splitting catalysts. The overpotential can be used as a measure of catalytic
activity. Yu et al.[23] prepared a nickel-based thin film (NiOx) on multi walled carbon nanotubes
deposited on ITO and observed an OER overpotential of 523 mV. Singh et al.[24]
electrodeposited layers of nickel oxide from [Ni(en)3]Cl2 (en= 1,2-diaminoethane) on glassy
carbon and reported 510 mV overpotential. Nardi et al.[25] deposited thin films of NiO Ni(Cp)2
(cp=cyclopentadienyl) on fluorine doped tin oxide (FTO) via atomic layer deposition and
achieved an overpotential of 400 mV. Lyons et al.[37] investigated the electrocatalytic activity
6
of polycrystalline nickel foils and reported an overpotential of 379 mV. Fominykh et al.[26]
prepared NiO nanoparticles using a solvothermal reaction in tert-butanol. Subsequently, NiO
nanoparticles were deposited on Au-coated QCM electrodes in order to access the OER
overpotential (280 mV). Trotochaud et al.[27] obtained a thin film of NiOx by spincoating a
solution containing Ni(NO3)2·6H2O on Au-coated QCM electrodes. Subsequent
electrocatalytic investigation in the OER regime revealed an overpotential of 279 mV.
McCrory et al.[38] published a comprehensive review on the electrocatalytic activity for
different metal oxide catalysts finding that the activity of NiOx catalysts can be further
enhanced by the addition of Fe. Gorlin et al.[30] synthesized Ni-Fe (62:38 at. %) catalysts with
a solvothermal approach and subsequently deposited them on carbon. Oxygen evolution
reaction activity was investigated in 0.1 M KOH revealing an overpotential of 0.25 V
(1 mA/cm²). Gong et al.[32] prepared a nickel-iron layered double hydroxide carbon nanotube
complex by a solvothermal method and showed an OER overpotential of 0.23 V (1 mA/cm²,
0.1 M KOH). Trotochaud et al.[33] electrodeposited thin films of Ni-Fe onto substrates and
subsequently investigated the OER activity revealing an overpotential of 0.27 V at 1 mA/cm²
(1 M KOH). A similar synthesis was conducted by Lu et al.[39] who electrodeposited Ni-Fe on
GC substrate and observed an OER overpotential of 0.31 V at 1 mA/cm² in 0.1 M KOH.
2.1.4 General aspects of acidic water splitting
Many problems arising for electrolysers working in alkaline media can be avoided when
operating under acidic conditions. For instance, the replacement of diaphragms with Nafion®
allows achieving higher current densities and better separation of product gases.[13]
Developed in the late 1960’s by Walter Grot of DuPont.[40-41] Nafion® is described as a teflon
derivate consisting of sulfonated tetrafluoroethylene polymer (PTFE) groups (Figure 2).
Figure 2: Nafion® was invented by Walter Grot of DuPont in the late 1960’s and is described as a polymer
typically deployed in electrolyser cells as a Proton Exchange Membrane (PEM). The polymer overcomes
typical problems observed for alkaline electrolysers, such as low pressure output, low partial load range
and low electric current densities.
C
F
2
F
2
C
CF
F
2
C
O
F
2
C
CF
O
C
F
2
F
2
C
xy
CF
3
S
O
O
HO
z
x H
2
O
7
Nafion® is applicable in two major fields of electro-catalysis. It can be dissolved in lower
aliphatic alcohols and subsequently used as a binder for attaching a catalyst powder on
substrates or used as a Proton Exchange Membrane (PEM) in acidic electrolyser cells
(Figure 3)
Figure 3: Proton exchange membrane (PEM) electrolyser cell usually consist of OER and HER catalysts
separated by a proton conducting membrane (e.g. Nafion®) embedded in gas diffusion layers and bipolar
plates. Water is fed at the anode side, whereas evolving O2 and H2 is released of the compartment at the
anode and cathode side, respectively.
The following half reactions are observed for a PEM electrolyser cell:
anode: 2 H2O O2 + 4 e- + 4 H+
cathode: 4 H+ + 4 e- 2 H2
overall: 2 H2O 2 H2 + O2
In general, PEM electrolyzer cells provide several advantages compared to alkaline
electrolysers. First of all, the Nafion membrane is as thin as 20 - 300 µm (commercially
available) and provides high proton conductivity between 0.083 and 0.16 S/cm.[42] This leads
to lower potential drop between the anode and cathode than for alkaline electrolysers.
Hence, current densities above 2 A/cm² can be achieved resulting lower operational costs.
Furthermore proton transport across the membrane responds very fast to the applied power
input, thus lowering the gas crossover rate and consequently increasing H2 purity in the
cathode chamber. In addition, no hazardous condition at low power input is reached in the
OER
catalyst
(Ir)
HER
catalyst
(Pt/C)
Membrane
Cathode
-
Anode
+
H
2
O
O
2
H
2
Gas
diffusion
layer
Bipolar plate
H
+
8
anode chamber. As a result, the operational range appears to be wider than for alkaline
electrolyser cells, whereby the nominal power density ranges between 10 - 100 %.
Electrolyser cells with a solid electrolyte allow a compact system architecture featuring
resistant structural properties allowing operation at high pressure.[43-44] This grants an
important benefit to the end user, who does not have to apply an additional amount of energy
in order to compress the evolved H2 gas. Furthermore, working under high pressure lowers
the specific volume of produced gas thus providing better gas removal.[13]
Even though acidic electrolyser cell provide plenty of advantages, some negative aspects
must be considered. Cross-diffusion of evolved gas in the respective opposite reaction
chambers is still present. Working pressures exceeding values higher than 100 bar further
enhance cross diffusion and usually requires the use of thicker membranes and internal gas
recombiners in order to prevent formation of hazardous gas mixtures. Furthermore, deployed
catalysts, current collectors and separator plates must withstand harsh working environment
characterized by low pH values, high applied potentials (>2 V) and high current densities.
Only a few materials can be applied to operate under such working conditions, e.g. noble
metal as catalysts as well as current collectors and separator plates based on titanium.
Water electrolysis is characterised by the Oxygen Evolution Reaction (OER) occuring at the
anode and the Hydrogen Evolution Reaction (HER) proceeding at the cathode. Typical
electrolysers are limited by the OER due to the fact that four electrons are needed to produce
one molecule of oxygen and that the OER proceeds by a complex reaction mechanism.
[13, 45-47] Active and stable catalysts with high accessible surface area can minimize the
overpotential required for both reactions[47] and potentially lower the amount of noble metal
thus decreasing investment cost of PEM electrolyser cells.
2.1.5 OER catalysts used in acidic media
A wide range of materials are used for the OER reaction, such as mixtures of IrO2/SnO2,[48]
IrO2/Ta2O5,[49] IrO2/Nb2O5,[50] IrO2/RuO2.[51] However, oxides of ruthenium and iridium show
the lowest OER overpotential in acidic media.[13, 52-53] Although ruthenium oxide shows higher
activity,[54] it typically corrodes during OER potential cycles.[55-56] Attempts were made in order
to stabilize RuO2, such as implementing 20 % IrO2 within RuO2. The corrosion rate of the
compound was successfully reduced to 4 % of the original value.[53] Iridium oxide is therefore
the best compromise for an active and stable OER catalyst.[13] Iridium oxide catalysts can be
prepared in different ways. Johnson et al.[57] dropcasted a solution containing iridium acetate
and isopropanol onto a titanium cylinder, followed by heat treatment at 480 °C.
Electrochemical testing in 0.1 M HClO4 indicated overpotentials of about 0.24 VRHE at a
9
current density of 1 mA/cm². Hu et al.[58] synthesized macroporous IrO2 utilizing colloidal SiO2
as pore template. Electrochemical testing in 0.5 M H2SO4 indicated 0.25 VRHE overpotential at
a current density of 1 mA/cm². Kushner-Lenhoff et al.[59] synthesized iridium oxide layers by
electrodepositing organic precursors Cp*Ir(H2O)3]2+ (Cp* = pentamethylcyclopentadienyl).
OER yielded overpotentials of about 0.267 V at 0.5 mA/cm². A similar synthesis by
Blakemore et al.[60] obtained a catalyst with approximately 0.270 V overpotential (at
0.5 mA/cm²). Oh et al.[61] prepared antimony doped tin oxide (ATO) with a sol-gel and
hydrothermal method. A solution containing H2IrCl6·xH2O, TTAB, water and NaOH was
heated to 70 °C and NaBH4 was added. The solution was cooled down and centrifuged in
order to obtain colloidal iridium nanodendrites. The as prepared colloids were washed,
dispersed in an ethanolic solution and finally deposited on an ATO support. Electrocatalytic
investigations were performed in 0.05 M H2SO4 observing an OER overpotential of 0.27 V at
1 mA/cm². A different approach was pursued by Nong et al.[62] who dealloyed a bimetallic
IrNix alloy precursor. The obtained IrNix@IrOx nanoparticles showed a core-shell architecture
and were deposited on mesoporous ATO. Electrochemical investigations were performed in
0.05 M H2SO4 showing an OER overpotential of 0.26 V at 1 mA/cm². Films of iridium oxide
and nickel oxide were synthesized by Reier et al.[63] via spincoating a solution containing
iridium acetate and nickel acetate tetrahydrate on titanium substrates. The as prepared
samples were heat treated at 450 °C and electrochemically investigated in 0.1 M HClO4. The
catalytic testing revealed an overpotential in the OER of 0.258 V at 1 mA/cm².
In general, iridium oxide catalysts with i) low crystallinity[64] and ii) high surface area[65] are
suggested to be more active for oxygen evolution. These characteristics can either be
adjusted by applying a moderate calcination temperature or by introduction of porosity into
the catalyst.
However, limited abundance and competition with other applications such as
supercapacitors,[66-67] stimulating neural electrodes[68-69] and microelectrodes for pH
sensing[70-71] require the most efficient utilization of IrO2 possible.[47] Many studies were
conducted on determine optimal synthesis conditions for iridium based OER catalysts. Some
of the most important findings are discussed in the chapters 2.1.6 - 2.1.8.
10
2.1.6 Basic investigations on iridium oxide - role of layer thickness
Johnson et al.[57] investigated the influence of layer thickness on electrochemical active
surface area and OER activity. They prepared, a solution containing Ir(OAc)3 and isopropyl
alcohol. Subsequently, a thin layer was prepared on a titanium substrate by spincoating,
whereas a thick layer was obtained by a dropcasting procedure. Afterwards, the samples
were heat treated at 480 °C in air. Catalyst layers were 17 -19 nm on silicon and even thinner
on titanium. An exact value for the titanium supported layer was not reported. However, the
layer thickness of dropcasted samples was not measured. XRD measurements were
conducted for thin and thick IrOx layers on titanium substrates. The thin IrOx layer showed
significant oxidation of the titanium susbtrate to TiO2, whereas no oxidized titanium was
observed for the thick layer. The authors conclude that, the IrOx layer is shielding the
underlying titanium susbtrate thus preventing oxidation. Investigations of the electrocatalytic
properties showed a 50-60 times higher electrochemical active surface area as well as higher
OER activity for the thicker IrOx layer. Furthermore, normalisation of the OER activity with
respect to the electrochemical active surface area showed a higher intrinsic OER activity for
the thicker IrOx layer related to the absence of an insulating TiO2 interlayer.
The work from Johnson et al. depicts two major advantages for thick IrOx layer on titanium
substrate. At first, they provide higher electrochemical surface area thus higher OER activity.
Furthermore, thick IrOx layers sufficiently prohibit oxidation from underlying titanium susbtrate
to TiO2 consequently providing a higher intrinsic OER activity.
2.1.7 Basic investigations on iridium oxide - role of calcination temperature
The impact of calcination temperature on structural properties of IrOx and electrocatalytic
OER activity was investigated by Reier et al.[64]. Similar to Johnson, a solution containing
Ir(OAc)3 and EtOH was spincoated on titanium coated silicon substrates. Subsequently, heat
treatment was conducted at temperatures ranging from 250 to 550 °C in air. Afterwards,
morphology, crystallinity and chemical state of IrOx was investigated as a function of
calcination temperature. A layer thickness of ~55 nm was found for samples calcined
between 250 and 450 °C, whereas calcination at 550 °C leads to thicker layers indicating
migration from titanium into the IrOx layer. Furthermore, XRD measurements were conducted
and showed higher IrOx crystallite size for samples calcined at higher temperaure. Samples
calcined at 350 °C exhibit the highest OER activity and electrochemical active surface area.
Calcination at 550 °C leads to oxidation of the underlying titanium substrate and enhances
diffusion of TiOx into the IrOx layer consequently leading to higher electrical resistivity
throughout the film volume and to reduced electrocatalytic OER activity.
The work from Reier et al. is of fundamental importance. It showed higher OER activity for
IrOx with smaller crystallite size. Furthermore, negative aspects of insulating TiO2 are
11
underlined and in good agreement with the observations made by Johnson et al. However,
the impact of TiO2 on electrical conductivity was not investigated in detail.
2.1.8 Basic investigations on iridium oxide - role of electrical conductivity
The influence of electrical conductivity on electrocatalytic activity was investigated by
Marshall et al.[72], by preparing a colloidal dispersion from metal precursors (i.e. H2IrCl6·4H2O
and SnCl2·2H2O) in ethylene glycol. After heating under reflux at a constant pH value of 2.5
the dispersion was centrifuged in order to obtain colloids. The colloids were then dried and
calcined in air at 500 °C. Subsequently, X-ray diffraction measurements revealed a rutile
structure with altering lattice parameters as a function of tin content indicating the formation
of a solid solution of iridium oxide and tin oxide. Electrical resistivity of the powder was
investigated and showed an increase of resistivity depending on the Sn content. Finally, the
electrochemical activity of the powder was investigated in a PEM electrolyser cell. The
activity normalized to the electrochemical active surface area remains high until a tin content
of 50 - 60 mol %, whereas a higher tin content leads to a remarkable drop of intrinsic activity.
The work from Marshall[72] thus underlines that highly active electrocatalysts are obtained
solely by providing a sufficient degree of conductivity.
Furthermore, Chen et al.[73] claims that high electrical conductivity is necessary in order to
provide a stable Ir-based catalyst on titanium substrate. Usually, low electrical conductivity
results in high electric fields throughout the coating causing quick migration of O2- species
through the substrate. Migrating O2- may then have a severe impact on the oxidation of the
underlying titanium substrate. Oxidized titanium leads to an additional ohmic loss thus
lowering the electro catalytic activity. The catalysts further lose activity with ongoing
passivation.
Comninellis et al.[74] studied the impact of electrical conductivity on electrocatalytic OER
activity. A metal salt solution containing at least one of the following compounds H2IrCl6,
RuCl3, TaCl5 or ZrOCl2 was coated on titanium and subsequently heat treated in air at
temperatures below 560 °C. The resulting microstructures of IrOx-TiO2, IrOx-ZrO2 and IrOx-
Ta2O5 were analyzed in terms of crystallinity, conductivity as well as OER activity. It was
found, that the obtained oxides showed low miscibility indicating a distribution of the
respective metal oxide clusters. Taking into account that TiO2, ZrO2 and Ta2O5 possess poor
electrical conductivity, whereas IrO2 shows metallic conductivity[54, 75-76] it was concluded that
electric conductivity is established by chains of conducting IrO2 clusters (percolation theory).
An insufficient amount of IrO2 in the catalyst leads to interruption of conducting chains,
causing a drop of electric conductivity as well as OER activity. Therefore, a significant
12
amount of metallically conductive metal oxide (i.e. IrO2) must be added in order to provide a
sufficient degree of conductivity that is beneficial for retaining highly active OER catalysts.
Another study investigated the mechanism of electron transport through a catalytic layer.
Oakton et al.[77] synthesized mixed metal oxides of IrO2/TiO2 by a simple one-pot Adams
method route. TiOSO4·0.6H2SO4·1.3H2O was dissolved in water along with H2SO4 and
IrCl3·3H2O. Afterwards, NaNO3 was added to the solution. The solution was dried in a rotary
evaporator and subsequently heat treated at 150 °C for 2h and 350 °C for 1 h. The obtained
powder was washed with water, dried and used for physicochemical and electrochemical
characterization. X-ray diffraction patterns of 40 % IrO2 - 60 % TiO2 revealed the presence of
three different oxides, i.e. TiO2 anatase, TiO2 rutile and IrO2 rutile. TEM images of the
corresponding sample in bright field mode showed IrO2 nanoparticles with 1 nm in diameter
deposited on TiO2 particles with a diameter of ca. 5 nm. The observed electrical conductivity
exponentially increased as a function of iridium content (TiO2: 2.3·10-8 S/cm, IrO2: 3.9 S/cm).
Percolation theory is a well known model to describe the electrical conductivity of randomly
packed particles with high and low electrical conductivity. The so called percolation limit
describes the minimal volume percentage that is required to form a conductive network.
Oakton determined a percolation limit of 35 % and observed an onset of electrical
conductivity for samples with iridium loadings higher than 35 mol % Ir (0.2 S/cm).
Further quantification of conductivity can be achieved by measuring sheet resistivity of
catalyst layers coated on insulating substrates such as glass. Furthermore, electrochemical
methods can be used in order to elucidate electron transport through bulk materials.
Stoerzinger et al.[78] deposited LaCoO3 on three substrates (with different conductivity) by
pulsed laser epitaxy in order to study the impact of conductivity on electron transport through
the layer by analyzing the peak positions of the [Fe(CN)6]3-/4- redox couple. They observed
enlarged distances of redoxpeaks spreading away from the equilibrium potential for samples
with low conductivity. Hence, samples with high resistivity cause a large voltage drop over
the layer leading to a lower voltage which promotes catalysis.
The literature survey from the chapters 2.1.6 - 2.1.8 underlines the influence of critical
reaction parameters that control the OER activity of iridium based catalysts. It can be
concluded that, the iridium based catalytic layer should preferentially be thick, amorphous,
electrically conductive and possess a high electrochemical active surface area in order to
operate as a highly active OER catalyst.
13
2.2 Oxides with templated porosity
Porous materials are used for different applications in industry and everyday life. Zeolites are
one of the most popular materials and used in washing powder. The properties of
mesoporous materials are presented in a very general manner in chapter 2.2.1. Different
synthesis approaches for the preparation of mesoporous materials are introduced in chapter
2.2.2 and the utilization of amphiphilic surfactants (chapter 2.2.3) i.e. amphiphilic block
copolymers (chapter 2.2.4) will be discussed in more detail. The synthesis of mesoporous
metal oxides with high pore ordering through self assembly of block copolymers (chapter
2.2.5) surrounded by suitable metal oxide precursors (chapter 2.2.6) will be described. The
self assembly of polymer templates can be triggered by exceeding the critical micelle
concentration achieved by ongoing solvent evaporation (EISA, chapter 2.2.7). A final
treatment decomposes the polymer template and converts the precursor into a mesoporous
metal oxide with a nanocrystalline structure (chapter 2.2.8).
2.2.1 Properties of mesoporous materials
Mesoporous systems are described as solid phase materials fully composed of pores. In the
case of connected pores the materials are considered as open porous materials providing
higher inner surface areas than bulk materials. This paves the way for different applications
in the field of catalysis and sorption. Zeolithes are the most prominent porous materials first
used by Henkel in 1977 for water softening. IUPAC classifies porous materials into 3 different
categories[79] according to their pore size.
microporous: < 2 nm
mesoporous: 2 - 50 nm
macroporous: > 50 nm
Microporous and mesoporous systems usually provide sufficient high surface areas for
catalytic processes. A major drawback for microporous and small mesoporous materials is
the occurrence of transport limitation processes during catalysis. Therefore, larger pore
diameters must be incorporated in order to provide sufficient product removal.[80] Mesoporous
systems are distinguished in unordered and ordered materials, both derived by different
synthesis approaches. The most relevant approaches for the introduction of mesoporosity in
materials are discussed in chapter 2.2.2.
2.2.2 Synthesis approaches for mesoporous oxides
Two different synthesis approaches are available in order to obtain mesoporous templated
materials. Endotemplating usually is characterized by a preliminary stage material that is
14
later surrounded by the mesoporous material precursor, whereas exotemplating first requires
a solid compound with cavities that can be later filled with precursor solution. A subsequent
template removal by etching or thermal treatment obtains the final porous material with a
high surface area (Figure 4).
Figure 4: The a) endo- and b) exotemplating approaches are characterized by the utilizaton of a template
(brown), the occurrence of intermediates (light blue) and the synthesis of a porous material (blue). a)
Endotemplating features the introduction of template in an arising solid material, whereas b)
exotemplating is characterised by the infiltration of a solid template with precursor solution.
Independently of the approach, both routes provide porous materials as a product. (Scheme based on the
work of Ortel[81])
The endotemplating approach is usually used for the synthesis of mesoporous oxides. Within
the approach, the preliminary stage material is a polymer that forms micelles within the metal
oxide precursor solution. After the condensation of the precursors into a “mesophase”, a
thermal treatment will remove the micelles and transform the precursor into a porous metal
oxide. The prior enclosed micelles provide an accessible pore system leading to a porous
metal oxide with high surface area.[82] The characteristics of the pore system such as pore
diameter and pore ordering can be easily tuned by an appropriate choice and concentration
of surfactant. Chapter 2.2.3 introduces the most common class of polymers (i.e. amphiphilic
block copolymers) used for the preparation of mesoporous metal oxides via endotemplating.
2.2.3 Amphiphilic surfactants
Amphiphilic surfactants exhibit a hydrophobic and hydrophilic part leading to versatile
reaction behaviours. The hydrophobic part consists of a large uncharged hydrocarbon
moiety, such as CH3(CH2)n with n > 4 and potentially contains alcohols or ethers, whereas
the hydrophilic part can be either ionic or non ionic. Ionic surfactants are subcategorised into
anionic (e.g. RCO2-) and cationic surfactants (e.g. RNH3+), where R presents the hydrophobic
part of the surfactant. Non ionic or uncharged surfactants usually contain alcohols with large
R groups. Amphiphilic surfactants contain a variety of subcategories, wherein the amphiphilic
a) Endotemplating
approach
b) Exotemplating
approach
15
block copolymers are from particular interest. Therefore, chapter 2.2.4 presents important
aspects related to amphiphilic block copolymers
2.2.4 Amphiphilic block copolymers
Amphiphilic block copolymers are the main building blocks for the preliminary stage materials
of the endotemplating approach. They are defined as an arrangement of covalent connected
polymers with different composition[83] and are divided in different types, such as diblock
copolymer and triblock copolymer. Figure 5 schematically shows the bonding characteristics
of diblock and triblock copolymers.
Figure 5: “Typical block copolymers” - Diblock and triblock copolymer with the main building block “A”
and “B”. Exemplarily, “A” might consist of a water soluble polymer such as polyethylene oxide (PEO),
whereas “B” is potentially composed of a water insoluble polymer like polypropylene oxide (PPO). BASF
developed such polymers in the 1950’s and still sell them under the tradename Pluronic®. For instance,
Pluronic® F127 is described as PEO106-PPO70-PEO106.
The amphiphilic block copolymers that are used for generating ordered mesoporous
materials mostly contain polyethylene oxide (PEO) as a hydrophilic part. Furthermore, a vast
amount of block copolymers are known in literature:
PS-b-PEO,[84-88] PI-b-PEO,[89-91] PMMA-b-PEO,[92] PHB-b-PEO (KLE),[93-95] PIB-b-PEO,[96-97]
PEO-b-PB)[97] and PEO-b-PB-b-PEO,[98] as well as commercially available block copolymers
like Pluronic® P123 (PEO20-PPO70-PEO20; Mw = 5800 g/mol) and Pluronic® F127 (PEO106-
PPO70-PEO106; Mw = 12600 g/mol).
All these amphiphilic block copolymers possess a variety of properties in solution according
to their structure and concentration, which directly influence the architecture of the
synthesized material. The most important characteristics of amphiphilic block copolymers
used for the synthesis of mesoporous materials will be highlighted in chapter 2.2.5.
A
AAB
B B B
B
A
A
Diblock copolymer
Triblock copolymer
A
AAB
B B B
B
A
A
A
AAAA
16
2.2.5 Critical micelle concentration and self assembly of block copolymers
Block copolymers in solution with a concentration below it’s critical micelle concentration
(CMC) are dissolved and randomly distributed. Exceeding the CMC significantly changes the
properties of the isotropic solution. The dissolved block copolymers form aggregates in order
to minimize their free energy. These aggregates usually shield the hydrophobic part in the
inside of the micelle, whereas the hydrophilic part keeps contact with the solution. A further
increase of polymer concentration caused by lower amounts of solvent between the micelles
results in rearrangement and various mesophases.[99] Figure 6 exemplarily shows different
mesophases potentially formed by amphiphilic block copolymers.
Figure 6: “Self assembly of block copolymers” - A large variety of different phases are formed by block
copolymers, e.g. spherical, cylindrical micelles with face centered cubic (fcc) and body centered cubic
packing (bcc). Image taken from Bucknall[100] with granted permission from The American Association for
the Advancement of Science.
Figure 6 shows the self organization of block copolymers possessing the capability to form
spherical and cylindrical micelles, vesicles, spheres with face-centered (fcc) cubic and body
centered cubic (bcc) packing, hexagonally packed cylinders, minimal surfaces (gyroid, F
surface, and P surface), simple lamellae, and modulated and perforated lamellae.[100]
The self organization is further exploited in the endotemplating approach by using polymers
as the preliminary stage material along with metal oxide precursor (see Figure 4). The
combination of a metal oxide precursor, and a polymer exhibiting the capability to form an
17
ordered mesophase is a well known technique in literature[94, 101-103] for the preparation of
mesoporous oxides. Chapter 2.2.6 describes fundamental aspects of one popular metal
oxide precursors, i.e. TiCl4. The rearrangement of polymers to highly ordered mesophases is
often achieved by exceeding the critical micelle concentration triggered by ongoing solvent
evaporation. The so called evaporation induced self assembly is an important tool for the
simple preparation of mesoporous metal oxides and explained in detail in chapter 2.2.7
2.2.6 Hydrolysis and condensation of metal oxide precursors
Suitable precursors must be utilized in order to obtain mesoporous templated compounds.
The metal oxide precursor usually is dissolved and subsequently interacts with solvent
molecules. A general reaction scheme is described as followed:
Hydrolysis: M-X + H2O M-OH + HX
Condensation: M-OH + M-OH M-O-M + H2O
Where M = metal centre and X = halide
First, hydrolysis takes place wherein the metal halide reacts with water to form a hydroxide
species under the release of a halide acid. Afterwards, the obtained metal hydroxide species
reacts with itself forming a metal oxide bridged network. Reports in literature describe TiCl4
as a suitable precursor for the synthesis of mesoporous templated TiO2.[99, 102, 104-105] A
general reaction scheme for TiCl4 performing hydrolysis in a solution of ethanol and water
was published for instance by Pan.[99]
TiCl4 + x EtOH + y H2O TiCl4-x-y(OEt)x(OH)y + (x+y) HCl
Hydrolysis of TiCl4 takes place under the release of HCl triggering hydrolysis. Moreover, the
hydrolysed titanium species can undergo condensation reaction thus forming an oxygen
bridged metal network under the release of EtOH. The release of HCl during hydrolysis of
TiCl4 in solution of EtOH/H2O induces strong acidic environments. As a result, further
hydrolysis of TiCl4 or even polycondensation of partially oxygen bridged titanium species is
suppressed. The obtained species exhibit small molecular mass and are present as inorganic
oligomers in the sol dispersion. Titanium oligomers[106-107] under acidic conditions are
stabilized and terminated by hydroxide groups. They are referred to as nano building blocks
(NBB) due to the interaction of the hydroxide groups with the hydrophilic part of the block
copolymer micelles through hydrogen bonding.[99, 102, 108]
18
The last chapters pointed out typical characteristics of polymers (chapters 2.2.3 - 2.2.5) and
metal oxide precursors in solution (chapter 2.2.6). Moreover, the interaction between both
reactants was introduced (chapter 2.2.6). The following chapter (2.2.7) depicts the
combination of both reactants in an endotemplating approach for the preparation of a
mesoporous templated metal oxide.
2.2.7 Evaporation Induced Self Assembly (EISA) exemplarily explained with TiO2
The so called evaporation induced self assembly (EISA) requires a solution containing block
copolymers (e.g. PEO-PB-PEO[98, 109]) and metal oxide precursors (e.g. TiCl4,[98] TALH[109]).
The EISA process is described as a combination of the i) cooperative liquid crystal template
(CLCT) mechanism[99, 110] and the ii) true liquid crystal template (TLCT) mechanism[99, 110]
taking place at two different stages during film preparation i) initial sol solution preparation
and ii) film deposition and aging. Therefore, EISA is divided into two stages according to the
present mechanism.[99, 110]
i) Preparation of sol solution (cooperative liquid crystal template mechanism, CLCT)
A homogenous dispersion of block copolymer and inorganic precursor (e.g. TiCl4) is prepared
in a volatile solution (e.g. EtOH/H2O). In general, the inorganic precursor immediately reacts
in terms of hydrolysis and condensation.[99] Thus, leading to the formation of HCl and small
inorganic oligomers terminated by hydroxide groups referred to as nano building blocks
(NBBs, chapter 2.2.6).[106-107] The HCl formation causes an acidic environment consequently
suppressing further polycondensation of NBBs. Subsequently, the partially hydrolyzed
titanium species interact with hydrolytic regions of the block copolymers through hydrogen
bonding.[99, 102, 108] This cooperative liquid crystal template (CLCT) mechanism leads to the
formation of titanium oligomers attached to the block copolymers.
ii) Film deposition and ageing (true liquid crystal template mechanism, TLCT)
The as prepared solution is characterised by a dissolved polymer interacting with dissolved
metal oxide precursors through hydrogen bonding. The solution is now used for film
deposition on suitable substrates such as silicon or titanium. Dipcoating appears to be a
convenient method due to control of temperature, humidity and withdrawal rate.[111]
Immersion and consecutive dragging out of the substrate from the solution triggers several
processes. The continuous evaporation of the solvent induces an increase of polymer- and
metal oxide precursor concentration. At first, the enrichment of the block copolymer induces
phase segregation between the hydrophilic and hydrophobic part. After exceeding the critical
micelle concentration the block copolymers self assemble to micelles (TLCT).[99, 110] At
19
second, other volatile compounds besides EtOH evaporate (e.g. HCl). Thus, leading to an
increase of pH-value and consequently triggering the thermodynamically favourable
condensation and polycondensation reactions of the hydrolysed metal oxide precursor (sol-
gel process). Finally, a connected amorphous metal oxide network is formed around the
highly ordered self assembled micelles.[99]
Figure 7 schematically illustrates the evaporation induced self assembly of block copolymers
and metal oxide precursors during dipcoating.
Figure 7: Schematic illustration of the Evaporation Induced Self Assembly (EISA). A volatile solution
containing a block copolymer and metal oxide precursor is prepared. The substrate is immersed in
solution and consequently dragged out. Evaporation of solvent and HCl (in case of TiCl4) leads to
enrichment of the polymer and precursor concentration inducing self assembly of the polymers and
polycondensation of the oxide precursor. In the end, a connected amorphous metal oxide network is
formed around the ordered micelles.
A variety of different porous metal oxide compositions have been prepared by the
evaporation induced self assembly process. Chapter 2.2.8 presents the transformation of the
arranged spherical micelles surrounded by metal oxide precursor into a mesoporous
templated material.
Micelle-precursor-film
„mesophase“
Substrate
Evaporating
solvent
Polymer
Dissolvedprecursor
Withdrawal
direction
20
2.2.8 Transformation of ordered mesophases to mesoporous oxides
The micelle-precursor films prepared according to the procedure described in chapter 2.2.7
are subsequently dried at temperatures between 60 - 200 °C[99] in order to grant full
polycondensation of nano building blocks leading to a more stable mesophase. Afterwards,
heat treatment at higher temperatures is performed to transform micelle-precursors into a
mesoporous templated metal oxide with nanocrystalline structure. In case of Pluronic F127
(PEO106-PPO70-PEO106; Mw = 12600 g/mol) the decomposition temperature was found to be
340 °C,[112] whereas Pluronic P123 (PEO20-PPO70-PEO20; Mw = 5800 g/mol) decomposes
around 220 °C.[113] Thermally induced crystal growth of pore walls composed of TiO2 is
observed for calcination at 350 °C.[114] Decomposition of pore template and transformation of
amorphous pore wall into a crystalline material typically is accompanied by film shrinkage
perpendicular to the substrate. Due to strong attachment of metal oxide precursor on the
substrate surface the occurring contraction of the film is only present perpendicular to the
substrate thus prevent cracking of the layer.[81, 99] In case of TiO2, a lower crystallization
temperature accompanied by less film contraction was observed for slow heating ramps of
0.5 - 2 °C/min.[115] Figure 8 illustrates the heat treatment process of a micelle-precursor-film
mesophase into a crystalline oxide with an accessible porous system.
Figure 8: General scheme for the synthesis of mesoporous templated metal oxides. The micelle-
precursor-film obtained by dipcoating (described in chapter 2.2.7) is thermally treated in air. Thus,
decomposition of micelles and transformation of the precursor into a metal oxide with nanocrystalline
structures takes place. Furthermore, template removal is accompanied by film shrinkage perpendicular to
the substrate.
Polymer templating is a powerful route to introduce mesoporosity in various metal oxides, i.e.
TiO2,[98, 116] IrO2,[65] NiO,[117] RuO2,[118] SnO2,[105] Nb2O5,[105] MgO.[103] Thus, the next chapters
describe different synthesis approaches for the preparation of Al2O3, MgO, Co3O4, ZnO (all
chapter 2.3.1), TiO2 (chapter 2.3.2), and IrO2 (chapter 2.3.3).
Calcination
Layer thickness
Substrate
Micelle
Precursor
Micelle-precursor-film
„mesophase“
Mesoporous templated
metaloxide
Meso-
pore
Nano-
crystal
21
2.3 Synthesis routes for metal oxides
The following chapter (2.3) introduces synthesis concepts based on different metal oxide
precursor systems for the preparation of mesoporous metal oxides such as Al, Mg, Co, Zn, Ti
and Ir. Chapter 2.3.1 presents a very simple and versatile approach for the successful
preparation of metal oxides from aluminum, magnesium, cobalt and zinc. The synthesis
succeeds by employing a metal complex formed from citric acid and metal nitrate along with
a triblock copolymer PEO213-PB184-PEO213 employed as a mesopore template. Chapter 2.3.2
introduces exemplarily different precursor concepts reported in literature to obtain
mesoporous templated titania. Finally, chapter 2.3.3 shows to the best of our knowledge, the
only synthesis concepts based on polymer templating for the preparation of mesoporous
iridium oxide.
2.3.1 Synthesis concepts for mesoporous Al2O3, MgO, Co3O4, ZnO - The “citrate route”
Eckhardt et al.[103, 119] presented a synthesis route which combines three different strategies
such as i) complexing the metal ion (Pechini method), ii) decomposing the carbonate and iii)
pore templating with polymer micelles. The approach tackle typical problems associated with
the building mechanism of mesoporous oxides, thus granting access to various metal oxide
and even carbonate compounds of Al,[119] Mg,[103] Co,[119] and Zn.[119]
Figure 9: Scanning electron microscopy (SEM) images of accessible mesoporous templated metal
carbonates and oxides of aluminium, magnesium, cobalt and zinc. All compounds were synthesized via
citrate route. (SEM images taken from Eckhardt et al.[103, 119] and reprinted with permission from the
American Chemical Society)
Five different boundary conditions must be fulfilled in order to provide a generalized
synthesis approach for metal oxides. Figure 10 illustrates the different requirements usually
associated with the synthesis strategy:
Remaining template
polymer prevents
imaging by electron
microscopy due to
instability of
the sample.
50 nm
MO
X
Al
M(CO
3
)
X
Mg Co
a) b) c)
e) f) g)
50 nm
Zn
h)
50 nm 50 nm 50 nm 50 nm
h)
50 nm
d)
22
1) Metal salts have to form a chemical complex with ligands containing carboxylic acid
functionality (e.g. citric acid). Moreover, chelating ligands are favored due to their higher
chemical stability.
2) The solution is coated onto a substrate leading to solvent evaporation. The containing
polymer should possess the capability of evaporation induced self assembly. Self assembly
is required for the successful formation of an ordered micelle-precursor-film mesophase.
3) The metal complex should show the ability to transfer into a carbonate at temperatures
below the descomposition temperature of the polymer template. Transformation of the metal
complex into a carbonate prior template removal is epecially important for preventing pore
structure collapsing thus providing stabilization of the micelle-precursor-film mesophase.
4) The pore template must be removed prior to metal carbonate decomposition in order to
obtain a mesoporous metal carbonate. Otherwise, the mesoporous structure of the metal
carbonate is not accessible due to the presence of pore template.
5) Finally, a calcination step is applied to decompose the metal carbonate consequently
leading to formation of nanocrystalline metal oxides with preserved pore structure.
Figure 10: The citric acid complexed metal nitrate synthesis route is shown together with the deduced
requirements (1-5). Necessary requirements for the successful preparation of mesoporous templated
metal oxides are as followed: 1) Formation of a soluble metal complex (i.e. metal nitrate and citric acid). 2)
Film deposition to induce self assembly of polymer template and obtain an ordered mesophase. 3)
Precursor decomposition and transformation of the complex into a structurally stable carbonate at low
temperatures under retaining the ordered mesophase. 4) Heat treatment in air to decompose polymer
template and generate mesoporous metal carbonate with accessible mesoporosity. 5) Heat treatment at
higher temperatures to transfer amorphous metal carbonates into nanocrystalline metal oxides under the
release of CO2 and preservation of the mesoporous system. Image taken from Eckhardt et al.[119] and
reused with the permission of the American Chemical Society.
Micelles
Mesoporous
metal oxide
Metal complex
M(CO3)x
PEO-b-PB-b-PEO
Mesoporous
metal carbonate
MOx
Micelle-structured
metal carbonate
Dip-coating solution
Metal nitrate
Polymer template
Citric acid
Micelle-structured
metal-complex film
Coating
T T T
Required:(1) Formation of a
soluble metal
complex
(2) Self-assembly into an
ordered mesophase
(4) Template removal without
mesopore collapse
(3) Transformation of the complex
into a structurally stable metal
carbonate at low temperatures
(5) Transformation of
carbonate into metal oxide
without mesopore collapse
Essential: Suitable thermal (in)stability of template,
metal complex and metal carbonate
23
In case of MgO[103] the metal complex is formed in solution by treating magnesium nitrate with
citric acid. The as prepared metal complex is transferred into a stable MgCO3 phase by
thermal treatment. Subsequently, a second calcination step at higher temperature leads to
decomposition of the carbonate and finally results in the formation of a mesoporous
templated MgO phase. The synthesis was conducted in ethanolic solution containing PEO-
PB-PEO triblock copolymer employed as a polymer template and a metal complex as an
oxide precursor. Dipcoating was performed on silicon substrate followed by calcination at 400
and 600 °C to obtain a mesoporous magesium carbonate and oxide. Another publication of
Eckhardt et al.[119] demonstrate the versatility of the citric acid approach by showing the
successful synthesis of micelle-templated oxides and carbonates of zinc, cobalt and
aluminium (see Figure 9 for corresponding SEM images).
2.3.2 Synthesis concepts for mesoporous TiO2
Several synthesis routes are available for the preparation of mesoporous templated TiO2.
Figure 11 exemplarily shows a selection of electron microscopy images of TiO2 obtained by
different metal oxide precursors such as a) Ti(iPrO)4, b) TiCl4, c) preformed TiO2 nanocrystals
and d) TALH.
Figure 11: SEM micrographs of mesoporous templated TiO2 synthesized from different precursors. a)
Antonelli et al.[120] prepared pre-stabilized titanium isopropylate with acetylacetonate and subsequently
introduced pore templating polymers. b) Yang et al.[105] achieved self-stabilization of titanium species by
providing intrinsically acidic environments through HCl, which is released by the reaction of TiCl4 in water
ethanol-rich solutions. c) Brezesinski et al.[95] first prepared TiO2 nanocrystals and subsequently added
KLE as a pore template. d) Ortel et al.[109] worked in non acidic conditions by employing lactic acid
complexed titanium (TALH) as a titania source and PEO-PB-PEO triblock copolymer as a mesopore
template. All pictures have been taken from the respective publications.
a) One of the first synthesis approaches to obtain mesoporous TiO2 was published by
Antonelli et al.[120] The authors prepared acetylacetonate stabilized titanium alkoxides such as
Ti(iPrO)4. The exclusion of the stabilizing agent (acetylacetonate) immediately led to
excessive hydrolysis and condensation reaction, thus precipitation of the oxide-alkoxide
aggregates. However, the stabilized titanium alkoxide was added to a solution containing a
Ti(
i
PrO)
4
+ stabilizer TiCl
4
TiO
2
nanocrystals TALH
a) b) c) d)
24
polymer template (e.g. tetradecylphosphate). After several synthesis steps including a final
heat treatment under air preserved the first hexagonally packed mesoporous TiO2 with a
surface area of 200 m²/g and a pore opening with 3.2 nm in diameter.
b) No stabilizing agent is necessary in the case of TiCl4 being utilized as a TiO2 source as it
provides self stabilization. The route was published by Yang et al.[105] and exploits the
formation of HCl during hydrolysis of TiCl4 in a water ethanol-rich solution. The formation of
HCl induces strong acidic environments thus suppressing further polycondensation of the
oxide-alkoxide aggregates. The stabilized titanium alkoxides are subsequently mixed with
suitable polymers (e.g. P123) and heat treated in air to obtain mesoporous templated TiO2 in
anatase phase with a crystallite size of 2.4 nm. Further physicochemical analysis revealed a
pore size of 6.5 nm and a BET surface area of 205 m²/g.
c) Brezesinski et al.[95] sythesized pre-formed TiO2 nanocrystals from TiCl4, EtOH and benzyl
alcohol. Afterwards, the obtained nanoparticles were redispersed in ethanol and
subsequently mixed with KLE as a pore template. Dipcoating and heat treatment in air at
600 °C leads to the formation of mesoporous templated TiO2 layers. The derived layers show
bimodal porosity with 1 - 4 and 20 - 25 nm diameter pores. Further physicochemical analysis
revealed a body centered cubic packing of the pore system and a BET surface area in the
range between 180 - 200 m²/g.
d) Moreover, Ortel et al.[109] prepared a solution of lactic acid complexed titanium (titanium(IV)
bis(ammonium lactato)dihydroxide abbreviated as TALH), polymer template (e.g PEO-PB-
PEO, F127), water and ethanol. Due to the high chemical stability of the metal complex no
hydrolysis and condensation reaction occur under non acidic conditions. Subsequently, the
solution was dipcoated on different substrates and heat treated in air. The prepared
mesoporous templated TiO2 showed high surface area, exhibited an anatase structure and
showed locally ordered mesopores with an opening of 13.5 nm (F127) and 29.4 nm (PEO-
PB-PEO) in diameter.
25
2.3.3 Synthesis concepts for mesoporous IrO2
Only a few precursor concepts for the preparation of polymer templated IrO2 is reported in
literature. Figure 12 shows different iridium oxide precursors used along with amphiphilic
block copolymers to obtain mesoporous IrO2.
Figure 12: SEM images of polymer templated IrO2 obtained by a) F127, K2IrCl6 and alkaline hydrolysis[121]
and b) PEO-PB-PEO and Ir(OAc)3. [65] Images were taken from the respective publications.
a) Chandra et al.[121] used PEO-PPO-PEO (F127) block copolymer as a pore template and a
monomeric [Ir(OH)6]2- complex obtained by alkaline hydrolysis of K2IrCl6 as an oxide
precursor. The solution was spincoated onto FTO substrate dried at 80 °C, annealed at
150 °C and finally heat treated at temperatures between 400 - 500 °C, respectively. Thicker
layers were obtained by multi spincoating with intermediate drying (80 °C) and annealing
(150 °C). Physicochemical analysis revealed a pore diameter of 7 nm, layer thickness of ca.
70 nm and BET surface areas between 65 m²/g (Tcalc. = 400 °C) and 105 m²/g (Tcalc. =
500 °C).
b) Ortel et al.[65] prepared an ethanol rich solution containing iridium acetate as a metal oxide
precursor and employed PEO-PB-PEO polymer as a pore template. The solution was
dipcoated on different substrates and consequently heat treated under air. The authors
reported a pore diameter of ~16 nm, rutile type structure, a locally ordered pore arrangement
and BET surface areas between 140 (Tcalc. = 300 °C) and 20 (Tcalc. = 700 °C) m² per m² of
geometric surface area.
Ir(OAc)3
b)
a)
K2IrCl6
26
2.4 Deduced thesis aim and approaches
The aim of this thesis is to obtain catalysts with higher electrocatalytic oxygen evolution
reaction activity compared to commercially available catalyst powders and to understand the
factors that control OER activity.
To achieve this goal the synthesis route presented for oxides of Al, Mg, Co, Zn (see chapter
2.3.1) is extended to Ni for electrochemical testing in alkaline media. The synthesis
approaches for IrO2 by Ir(OAc)3 (chapter 2.3.3) and TiO2 from TiCl4 and TALH (chapter 2.3.2)
are combined in order to obtain mesoporous templated layers of IrO2 and mixed metal oxides
IrO2/TiO2 with higher catalytic activity in acidic media compared to a commercial reference.
A controlled variation of synthesis parameters during the preparation of mesoporous
templated catalytic layers, i.e. NiO, IrO2, IrO2/TiO2 was performed. An extensive analysis for
the impact of synthesis parameters on structural properties and electrochemical activity was
performed. The obtained data were then evaluated in order to identify the optimal synthesis
conditions for the generation of highly active electrocatalysts. The varied parameters were: i)
calcination temperature, ii) iridium loading and iii) withdrawal rate.
i) Heat treatment conducted at different temperatures was used in order to study the effect of
crystallinity on intrinsic and overall OER activity. ii) A different amount of iridium oxide was
dispersed within TiO2 to obtain samples with different electrical conductivity. The different
electrical conductivity was then used to identify changes in electron transport mechanisms.
iii) By varying the withdrawal rate electrocatalytic coatings with different layer thicknesses
were obtained. The catalysts were used as a model type system to identify potential gas
removal limitation at high electrical current densities and potentials.
A comprehensive investigation and comparison of physicochemical and electrochemical
properties revealed that the overall OER activity is affected by several parameters such as
crystallinity, electrical conductivity and active surface area. However, no signs of transport
limitations were detected for systems with high layer thicknesses at high gas production
rates.
27
2.5 Thesis outline
Chapter 3 illustrates experimental data by offering information about the synthesis of
mesoporous templated catalytic coatings on different substrates (chapter 3.1). Moreover, the
applied physicochemical techniques (chapter 3.2) to determine structural properties and
electrocatalytic testing procedures (chapter 3.3) for quantifying the oxygen evolution reaction
activity and electrochemical accessible surface area are explained.
The results and discussion are presented in chapter 4. Chapter 4.1 describes a new
approach for the synthesis of NiO coatings with narrow pore size distribution and tunable
mesopore size. The synthesis is based on micelles of amphiphilic block copolymers
employed as a pore template and citric acid complexed metal compounds. The versatility of
the citrate based synthesis approach is confirmed by showing the accessibility of
homogeneous NiO coatings with templated and locally ordered mesoporous structure. The
electrochemical OER activity is investigated in alkaline media to deduce structure activity
relationships. Moreover, a comparison of OER activity with reports from literature is
provided.[122]
Chapter 4.2 exploits the potential of pore templating with polymer micelles in order to
produce model-type porous catalysts for the investigation of structure-activity relationships in
gas evolution reactions and for the optimization of the performance of IrO2-based OER
catalysts. The developed synthesis from Ortel[65] based on pore templating with micelles of
amphiphilic block copolymers PEO-PB-PEO[65, 98] is further improved to produce iridium oxide
films with controlled pore size, film thickness and crystallinity. The model systems are used to
study the influence of porosity and crystallinity on electrochemically accessible surface area
(ECSA), OER performance and gas transport. A controlled variation in thickness of the
porous catalysts explores, which parts of the catalyst can be utilized without transport
limitations during high-current OER. The combined knowledge is used to design a multilayer-
IrO2 catalyst that shows the lowest overpotential reported so far for monometallic oxide
compounds of Ir.[47]
Chapter 4.3 and 4.4 investigate two different synthesis routes for the preparation of mixed Ir
and Ti metal oxides. Both routes are based on a soft templating approach with PEO213-PB184-
PEO213 as a pore template, iridium acetate as an IrO2 source and either TiCl4 (chapter 4.3) or
TALH (chapter 4.4) as a titania precursor. The chemical properties of TiCl4 and TALH vary
from each other leading to different interaction with the dissolved polymer template thus
providing different morphological properties such as metal oxide distribution. The influence of
calcination temperature and iridium content for both synthesis routes is investigated in terms
28
of surface area, crystallinity, conductivity, morphology and OER activity. Correlations of the
obtained data are used to identify OER-controlling parameters for the successful preparation
of highly active OER electrocatalysts.
Chapter 4.5 illustrates the electrocatalytic performance of commercially available catalyst
powders. The purchased powders were deposited on the working electrode by a typical
“Nafion-ink” based synthesis approach. Electrocatalytic investigations were conducted in
order to identify the most active commercial powder. Moreover, the reproducibility of the ink-
based synthesis approach is shown by applying different iridium loadings on the working
electrode. The obtained data are used to determine the iridium mass based OER activity for
commercial reference catalyst powders.
Chapter 5 presents combined observations of systems used for electrochemical testing
under acidic condition, i.e. IrO2 and IrO2/TiO2. This general discussion is used to identify
general trends and deduce potential structure-activity relationships. Synthesis parameters
such as calcination temperature, crystallinity, electrical conductivity, electrochemical active
surface area (ECSA) and layer thickness were identified as the most relevant OER-
controlling parameters. Furthermore, the applied overpotential during electrocatalytic
investigation showed to possess an impact on kinetical aspects, i.e. Tafel slope. A
comprehensive study on observed structure-activity relations revealed high OER activities for
samples exhibiting low crystallinity, high electrical conductivity and large ECSA. Synthesized
catalytic coatings of IrO2 (chapter 4.2) and IrO2/TiO2 (chapter 4.3 (Ir(OAc)3 + TiCl4) and
chapter 4.4 (Ir(OAc)3 + TALH)) fulfilling the observed criteria are then used for comparison
with commercial catalytic powders (from chapter 4.5) in terms of iridium mass based OER
activity. The observed iridium mass normalized OER activity of polymer templated IrO2 and
IrO2/TiO2 appear to be at least 10 times higher than for commercially available catalysts.
29
3 Experimental
The present chapter (3) contains information about the synthesis of micelle-templated films
(chapter 3.1) and the applied analytical methods in order to determine morphology,
crystallinity, phase composition, surface area, pore ordering, surface composition and
electrical conductivity (chapter 3.2). Moreover, the electrocatalytic testing is described in
detail (chapter 3.3) offering information about the investigation of oxygen evolution reaction
(OER) activity and electrochemical active surface area (ECSA) in acidic and alkaline media,
respectively.
3.1 Synthesis of micelle-templated films
Dipcoating (Coater 5 AC, IdLabs Vesely) was used in order to deposit thin metal oxide films
on a suitable substrate. Different substrates were used for the investigation of certain
structural and catalytical properties: Physicochemical analysis was conducted for samples
coated on single side polished silicon wafers (SEM, XRD, TEM, SAED, XPS), double side
polished silicon wafers (physisorption), microscope slides (electrical conductivity), titanium
foil (SAXS) and titanium sheets/cylinders (SEM, XRD, TEM, SAED) Electrochemical
investigations were solely performed for layers coated on titanium sheets and cylinders
(OER, ECSA, DEMS). Prior to coating, silicon as well as titanium substrates passed through
different cleaning procedures. Silicon wafers, titanium foil and microscope slides were
washed with ethanol, whereas titanium substrates were firstly polished by SiO2-polishing
paste (Buehler, MasterMet 2, noncrystallizing colloidal silica suspension, 0.02 µm), then
ultrasonicated in water and eventually rinsed with ethanol (VWR Chemicals, 99.98 %
absolute).[122]
3.1.1 Mesoporous nickel oxide films
The solution for dipcoating was obtained by first dissolving 70 mg of a polymer template
poly(ethylene oxide)-b-poly(butadiene)-b-poly(ethylene oxide) (PEO213-PB184-PEO213,
containing 18 700 g mol-1 PEO and 10 000 g mol-1 PB, from Polymer Service Merseburg
GmbH)[65, 98] in 0.2 mL water (milliQ) and 2.8 mL ethanol. The solution was stirred for 12 h.
Subsequently, 144.1 mg of citric acid (Carl Roth, 99.5 % p.a.) and 436.0 mg of
Ni(NO3)2·6H2O (NeoLab, 98 %) were added.
The obtained green solution was transferred to a cuvette inside a dipcoater, where a
controlled atmosphere had been established with a temperature of 25 °C and a relative
humidity of 40 %. Dipcoating was performed at a withdrawal rate of 200 mm/min. Freshly
coated samples were dried for another 10 minutes under same conditions. Followed by two
subsequent heat treatments, the freshly synthesized samples were first thermally treated for
30
1 hour in a prehated drying oven at 250 °C and then calcined for 1 hour in a preheated muffle
furnace at 350, 400, 450 and 500 °C, respectively.
3.1.2 Mesoporous iridium oxide films synthesized from Ir(OAc)3
Mesoporous IrO2 films were synthesized on polished titanium cylinders following a procedure
established by Ortel et al.[65] Dipcoating solutions for calcination studies were obtained by
adding 225 mg Iridium(III) acetate (Heraeus, 48.76 % Ir content) and 45 mg of a polymer
template poly(ethylene oxide)-b-poly(butadiene)-b-poly(ethylene oxide) (containing
18 700 g/mol PEO and 10 000 g/mol PB, from Polymer Service Merseburg GmbH)[98] to a
volume of 1.5 mL ethanol. For thicker films and multilayers a volume of 1.3 mL EtOH and
0.1 mL H2O was used.
Dipcoating of single layer catalysts was performed under controlled atmosphere at a relative
humidity of 40 % and a temperature of 25 °C at a withdrawal rate of 100 mm/min in a
dipcoater. Films were calcined subsequently placing the samples for 5 min in a hot muffle
furnace with air atmosphere at temperatures between 325 and 625 °C, respectively. For the
controlled variation of film thickness the substrates withdrawal rate was adjusted between 10
and 150 mm/min using the same calcination routine (5 min, 375 °C). Multilayer catalysts
were obtained by repeated dipcoating (30 mm/min) and heat treating (30 min, 200 °C) of
individual layers followed by a final calcination step (5 min, 375 °C).[47]
3.1.3 Mesoporous mixed oxide films of Ir and Ti synthesized from Ir(OAc)3 and TiCl4
The dipcoating solution for the preparation of 30 wt. % Ir in Ir/TiO2 was obtained by dissolving
35 mg of a polymer template poly(ethylene oxide)-b-poly(butadiene)-b-poly(ethylene oxide)
(PEO213-PB184-PEO213, containing 18 700 g mol-1 PEO and 10 000 g mol-1 PB, from Polymer
Service Merseburg GmbH)[65, 98] in 1.25 mL ethanol (99.9 %, Roth) and 0.21 mL milliQ water.
Subsequently, a solution containing 1.25 mL EtOH and 93.3 µL of titanium(IV) chloride (TiCl4,
99.9 %, Sigma Aldrich) was added dropwise under stirring. Finally, 55.8 mg Ir(III) acetate
(Heraeus, 48.76 % Ir content) was added to the solution.
The obtained dark green solution was transferred to a cuvette inside a dipcoater, where a
controlled atmosphere has been established with a temperature of 25 °C and a relative
humidity of 40 %. Dipcoating was performed at a withdrawal rate of 200 mm/min on polished
titanium substrate. Freshly coated samples were dried for another 10 minutes under the
same conditions. Afterwards, the samples were calcined in a preheated muffle furnace for
10 minutes under air at temperatures between 200 to 600 °C, respectively.
31
3.1.4 Mesoporous mixed oxide films of Ir and Ti synthesized from Ir(OAc)3 and TALH
Solution for dipcoating a layer of 30 wt. % Ir in Ir/TiO2 was obtained by dissolving 35 mg of a
polymer template poly(ethylene oxide)-b-poly(butadiene)-b-poly(ethylene oxide) (PEO213-
PB184-PEO213, containing 18 700 g mol-1 PEO and 10 000 g mol-1 PB, from Polymer Service
Merseburg GmbH)[65, 98] and 55.8 mg Ir(III) acetate (Heraeus, 48.76 % Ir content) in 2.5 mL
methanol (Sigma Aldrich). Subsequently, 408.6 µL of Titanium(IV) bis (ammonium lactate)
dihydroxide solution (TALH, 50 wt. % in H2O, Sigma Aldrich) was added dropwise under
stirring.
Obtained dark green solution was transferred to a cuvette inside a dipcoater, where a
controlled atmosphere has been established with a temperature of 25 °C and a relative
humidity of 40 %. Dipcoating took place with a withdrawal rate of 200 mm/min on polished
titanium substrate. Freshly coated samples were dried for another 10 minutes under the
same conditions. Afterwards, the samples were calcined in a preheated muffle furnace for
10 minutes under air at temperatures between 200 to 600 °C, respectively.
3.1.5 Reference catalyst (IrOx/TiOx)
The dispersion for dropcasting a layer of commercial availabe IrOx/TiOx was derived by
suspending 5.4 mg of IrOx/TiOx powder (73.9 wt. % Ir in TiO2, “Elyst 750480”, Umicore) in
2.49 mL water (milliQ), 2.49 mL iPrOH (> 99.5 %, Roth) and 20 µL Nafion perfluorinated resin
solution (5 wt. % in lower aliphatic alcohols and water, contains 15-20 % H2O, Sigma
Aldrich). The dispersion was ultrasonicated for 15 minutes showing a black appearance
(“ink”). Subsequently, 5 µL of the ink was pipeted onto a polished titanium cylinder (A =
0.1963 cm²) under room temperature. The titanium cylinder was transferred into a preheated
furnace and dried at 60 °C for 5 minutes. The nominal loading of iridium metal on the titanium
cylinder amounts to ca. 4 µg (~20 µgIr/cm²). Higher loadings were achieved by multi
dropcasting (repeated pipeting of 5 µL several times) with intermediate drying steps at 60 °C
for 5 minutes. The procedure was used to produce nominal loadings (iridium metal) between
ca. 4 - 800 µgIr (20 - 4075 µgIr/cm²).
3.1.6 Reference catalyst (IrO2, Sigma Aldrich)
5 mg of commercially available IrO2 powder (99.9 %, Sigma Aldrich) was dispersed in
2.49 mL water (milliQ), 2.49 mL iPrOH (> 99.5 %, Roth) and 20 µL Nafion perfluorinated resin
solution (5 wt. % in lower aliphatic alcohols and water, contains 15-20 % H2O, Sigma
Aldrich). The suspension was ultrasonicated for 15 minutes showing black colour.
Subsequently, 3 µL of the dispersion was dropcasted onto a titanium cylinder followed by a
drying step in a preheated furnace at 60 °C for 5 minutes. The obtained IrO2 catalyst on a
titanium cylinder exhibit nominal loadings of 2.57 µgIr (13.1 µgIr/cm²).
32
3.2 Analytical methods
The present chapter (3.2) offers information about the spectrum of physicochemical
techniques used for determining the morphology (3.2.1: SEM, 3.2.2: TEM), crystallinity and
phase composition (3.2.2: SAED, 3.2.3: XRD), surface area (3.2.4: Kr-physisorption), locally
pore ordering (3.2.5: SAXS), surface composition (3.2.6: XPS), electrical conductivity (3.2.7),
iridium content (3.2.8: ICP-OES) and faraday efficiency (3.2.9: DEMS).
3.2.1 Scanning electron microscopy (SEM)
SEM images were obtained using a JEOL 7401F instrument with an accelerating voltage of
10 kV. To determine film thickness of mesoporous iridium oxide films, a ceramic knife was
used to scratch the layer followed by SEM imaging of tilted Ti cylinders. SEM images were
analyzed with ImageJ v1.43u[123] to derive film thickness and pore diameter.[47]
3.2.2 Transmission electron micrographs (TEM) and selected area diffraction (SAED)
TEM and SAED images were obtained with a FEI Tecnai G² 20 S-Twin at an accelerating
voltage of 200 kV. The film samples were scraped off from a titanium cylinder or sheet and
then collected with a TEM-grid.[47] TEM micrographs were obtained in brightfield and high
angle annular darkfield (HAADF, 3° tilt angle) mode. SAED images were recorded in
diffraction mode at a sample area of ca. 200 nm in diameter. During TEM operation the
electron dose was lowered by broadening the electron beam to prevent potential reduction of
metal oxide compounds.
3.2.3 X-ray diffraction (XRD)
XRD patterns were recorded with a Bruker D8 Advance instrument using Cu Kα radiation,
grazing incident for the incoming beam and a Goebel mirror. Scherrer equation was applied
to certain reflections in order to determine crystallite size for phases of IrO2 (110),[47] TiO2
rutile (110), TiO2 anatase (101) and NiO bunsenite (111) and (200).
3.2.4 Kr-physisorption
Surface area was measured with Kr physisorption at 77 K using the Autosorb-iQ automated
gas adsorption station from Quantachrome and samples coated on double side polished
silicon wafers. Prior to adsorption measurement the samples were degassed for 2 h at
150 °C in vacuum. The surface area was calculated via Brunauer-Emmett-Teller (BET)
method.[122]
33
3.2.5 Small angle X-ray scattering (SAXS)
NiO 2D small angle X-ray diffraction (SAXS) measurements were performed at BESSY PCB
beamline, using a wavelength of 1.5498 Å (8 keV), a 2D detector (981 x 1043 pixel) with a
sample to detector distance of 1920 mm. Samples were mounted on a moveable sample
holder, ensuring rotation of samples between 90° and 20° with respect to incident beam.
Investigated oxide and carbonate films were coated on thin silicon wafers (50 µm) and
analyzed in transmission mode at angles of β=90° or β=20° with respect to substrate
normal.[122]
IrO2 and IrO2/TiO2 2D SAXS patterns (small angle X-ray scattering) were recorded on a
Bruker Nanostar (three-pinhole collimation system) using a copper anode as X-ray source
(CuKα radiation), a 2D detector (2-D HI STAR 1024 x 1024 pixels) with a sample to detector
distance of 670 mm and employing a sample holder that enabled rotation of the sample
between 90° and 20° relative to incident beam. Respective oxide films were coated on thin
titanium foil and analyzed in transmission mode with a beam incident angle of β = 90° and
β = 20° with respect to the film surface.
3.2.6 X-ray photoelectron spectroscopy (XPS)
XPS measurements have been carried out with an ESCALab 200X photoelectron
spectrometer (VG Scientific, U.K.) for all samples. XPS were recorded at an angle of
emission of 0° using non-monochromatized Al Kα excitation. The Binding energy (BE) scale
was calibrated using the C1s component of aliphatic hydrocarbon at BE = 285.0 eV.[122]
Observed signals were finally associated with specific binding energies reported in literature
and listed in NIST Chemistry WebBook, NIST Standard Reference Database
3.2.7 Electrical conductivity
Electrical conductivity was measured for catalytic coatings on microscope slides with a
Keithley Model 6517B Electrometer employing a 8x8 pin probe head with an altering polarity
sequence of the pins. Light induced enhancement of conductivity observed for
semiconducting materials (e.g. TiO2) was avoided by measuring under dark environment.
Applied potential was varied between 1 V - 10 V and was increased by a factor of 1.2 for
each step. The recorded current response was plotted as a function of potential. The
observed slope corresponds to the electrical sheet conductivity and is expressed as
(Ohm/sq)-1. The volume conductivity of each catalytic layer can be derived by dividing sheet
conductivity by layer thickness (expressed as (Ohm·m)-1 or S·m-1).
34
3.2.8 Inductively coupled plasma - optical emission spectrometry (ICP-OES)
The iridium loading on titanium substrates (diameters: cylinder 5 mm; sheets 6 mm) was
determined by first suspending the sample in a mixture of 6 mL HCl (37 %, Roth), 2 mL
HNO3 (69 % Roth), 2 mL H2SO4 (96 %, Roth) and 40 mg NaClO3 (99.0 %, Alfa Aesar). The
obtained suspension was slowly stirred (130 rpm) for at least 3 hours under room
temperature and subsequently transferred into a microwave (Discover, SP-D, CEM
Corporation) for acid digestion at 180 °C (ramp 15 K/min, 40 min, 18 bar). 2 mL water (milliQ)
was added to the solution after completion of a cooling down period. The as prepared
solution was analyzed in a 715-ES-inductively coupled plasma system (ICP-OES, CCD
detector, Varian) in order to determine the iridium content.
3.2.9 Differential electrochemical mass spectrometry (DEMS)
The amount of formed gas products was assessed in separate DEMS experiments utilizing
mesoporous templated IrO2 coated onto titanium cylinders. The DEMS apparatus is partly
based on a design reported elsewhere[124] and consisted of an electrochemical flow cell
(0.5 M H2SO4, flow rate: 5 µL/s) connected via separation PTFE membrane to a PrismaTM
quadrupole mass spectrometer (QMS 200, Pfeiffer-Vacuum) equipped with two
turbomolecular pumps HiPace 80 operating the MS chamber at 10-6 mbar. The MS was
calibrated with a reference gas CO2 in N2/O2 (Linde, 75.04 % N2; 19.95 % O2; 5.01 % CO2).
Cyclovoltammetric measurements were conducted in the OER regime by cycling the
potential between 1.20 - 1.65 VRHE (6 mV/s) while recording the ion current for O2 (mass 32)
and CO2 (mass 44). The amount of evolved O2 and CO2 was calculated from the ion
currents.[47]
35
3.3 Electrocatalytic testing
The following chapter contains detailed information about the electrochemical setup (chapter
3.3.1) and measuring procedures to determine the OER activity in alkaline (chapter 3.3.2)
and acidic media (chapter 3.3.3), respectively. Moreover, the electrochemical active surface
area (ECSA) was assessed for samples tested under acidic conditions (chapter 3.3.3).
3.3.1 Electrochemical setup
Electrocatalytic testing was performed in a three electrode disc setup using a Biologic SP
200 potentiostat, a reversible hydrogen electrode (Gaskatel, HydroFlex®) as a reference and
a Pt-gauze (Chempur, 1024 mesh/cm², 0.06 mm wire diameter, 99.9 %) as a counter
electrode. All potentials in this work are referred to the reversible hydrogen electrode and are
iR corrected. The utilized electrochemical setup is schematically shown in Figure 13.
Figure 13: Electrochemical setup used for the determination of the oxygen evolution reaction (OER)
activity and electrochemical accessible surface area (ECSA). Catalytic layers of NiO, IrO2 and IrO2/TiO2
were deposited on titanium and served as the working electrode. Platinum gauze was used as a counter
electrode. The applied potential is referred to a reversible hydrogen electrode and corrected for iR drop.
Electrochemical testings were either performed with supporting electrolytes of KOH (alkaline, NiO) or
H2SO4 (acidic, IrO2, IrO2/TiO2).
All films coated on titanium cylinders or sheets (5 mm in diameter) were mounted on a
rotating disk shaft and served as a working electrode (n = 1600 rpm) using H2SO4 (Fixanal,
N
2
Reference
electrode
(RHE)
Luggin
capillary
Electrolyte
Counter
electrode
(Pt)
Working
electrode:
1600 rpm
Geometric surfacearea
duringelectrocatalytic
testing: 0.196 cm²
SP 200 potentiostat
3 Electrode set-up with
rotating disc electrode (RDE)
36
Fluka Analytical) or KOH (Sigma Aldrich, pellets, ≥85 %) as supporting electrolyte. The
electrolyte solution was purged with nitrogen prior to catalytic tests.
3.3.2 Alkaline procedure in KOH (NiO)
The OER activity was investigated by cyclic voltammetry in a potential window ranging
between 1.20 - 1.95 VRHE in 0.1 M KOH at a scan rate of 6 mV/s.[47, 122] Furthermore, NiO was
electrochemically activated[27] in 1.0 M KOH at a static applied potential of 1.75 VRHE for
5 hours. After every hour of chronoamperometric treatment an intermediated cyclic
voltammogram was conducted at a scan rate of 20 mV/s in order to assess increasing
oxygen evolution reaction performance as well as redox waves prior the OER onset. [47, 122]
3.3.3 Acidic procedure in H2SO4 (IrO2 and IrO2/TiO2)
The OER activity of mesoporous templated catalytic coating, i.e. IrO2 and IrO2/TiO2 was
investigated by cyclic voltammetry in a potential window ranging between 1.20 - 1.65 VRHE in
0.5 M H2SO4 at a scan rate of 6 mV/s.[47, 122] To analyze the electrochemically accessible
surface area (ECSA) the potential was sweeped between 0.40 and 1.40 VRHE at a scan rate
of 50 mV/s. Placing hydrous IrO2 in solution and alter the potential will change the valence
state of surface metal atoms. TiO2 shows no significant current response in the applied
potential range. Furthermore, a reversible proton inclusion mechanism can take place as
described by Trasatti et al.[125]:
IrOx(OH)y + δ H+ + δ e- IrOx-δ(OH)y+δ
The ECSA of iridium oxide and mixed metal oxides of iridium and titanium was then
quantified by determining the mean value of the integrated anodic and cathodic scan of the
resulting cyclic voltammogram.[47, 55, 125-126]
37
4 Results and discussion
The following chapter (4) presents the synthesis approach for each mesoporous templated
system, i.e. NiO, IrO2 and mixed metal oxides of IrO2/TiO2. Subsequent to the film formation
all samples were characterized physicochemical. The resulting data were evaluated and
used for the creation of structure models containing detailed information on morphology,
crystallinity, phase composition and surface area. Moreover, the catalytic coatings were
electrochemically investigated to identify the performance in oxygen evolution reaction and
quantify the electrochemical accessible surface area. The combined physicochemical and
electrochemical data are then used to deduce structure-activity relationships. Exploiting this
knowledge allows the design of highly active OER-electrocatalysts with iridium mass based
OER-activities at least 10 times higher with respect to commercial available OER-catalysts.
Chapter 4.1 describes an approach for the synthesis of NiO by a citrate based synthesis
approach. The electrochemical OER activity is investigated for NiO layers on titanium
substrate in alkaline electrolyte solution to deduce structure activity relationships and conduct
a comparison with OER activities reported in literature.
Chapter 4.2 presents the potential of pore templating with polymer micelles for the
investigation of structure-activity relationships in gas evolution reactions and for the
optimization of the performance of IrO2-based OER catalysts. The chapter revealed that the
OER performance of mesoporous IrO2 is controlled by at least two independent factors, i.e.
the accessible surface area and the intrinsic activity per accessible site.
Chapter 4.3 shows an extended approach for the preparation of mixed metal oxide layers
with adjustable crystallinity and conductivity. The synthesis is based on micelles of triblock
copolymers and two metal oxide precursors such as Ir(OAc)3 and TiCl4. Chapter 4.4
demonstrates a synthesis approach for designing an almost throughout mixed metal oxide
comprising IrO2 and TiO2. The films were obtained by using a synthesis based on triblock
copolymers and two metal oxide precursors with similar chemical properties, i.e. Ir(OAc)3 and
TALH. The obtained layers of both chapters (4.3 and 4.4) were characterized
physicochemical and electrochemical. The obtained data were correlated to reveal structure-
activity relations indicating that the overall OER activity and intrinsic reactivity is affected by
the active surface area and electrical conductivity.
Chapter 4.5 illustrates a reproducible synthesis approach and the electrocatalytic
performance of commercial available catalyst powders.
38
4.1 Mesoporous templated NiO synthesized from Ni(NO3)2 and citric acid
Chapter 4.1 demonstrates the synthesis of homogeneous NiOx coatings with a templated and
locally ordered mesopore structure and their catalytic behaviour in alkaline OER.
Mesoporous NiCO3 and NiO films were obtained by deposition of Ni(NO3)2 in presence of
citric acid and the mesopore template poly(ethylene oxide)-b-poly(butadiene)-b-poly(ethylene
oxide) (PEO213-PB184-PEO213). Chapter 4.1.1 shows the thermal stability of the polymer
template and the nickel precursor investigated by thermogravimetric analysis (TGA) in order
to derive suitable parameters for calcination of deposited films. The influence of calcination
temperature on morphology, pore ordering and crystallinity of NiO and NiCO3 layers were
studied by scanning electron microscopy (SEM), transmission electron microscopy (TEM)
small angle X-ray scattering (SAXS), selected area electron diffraction (SAED) and X-ray
diffraction (XRD). The surface composition of the films was analyzed by X-ray photoelectron
spectroscopy (XPS) (chapter 4.1.2). Differently calcined catalysts were tested in alkaline
OER and studied by Kr-physisorption in order to deduce a direct relationship between OER
activity and accessible surface area (chapter 4.1.3). Electrochemical activation studies
similar to procedures reported in literature[27] resulted in further catalyst activation (chapter
4.1.4). Calcination at 350 °C produced NiO with low crystallinity yet high BET surface area
and resulted after further electrochemical activation in the highest OER activity. The most
active catalyst was further used for comparing the OER activity with reports from literature
(chapter 4.1.5).
4.1.1 Thermal behavior of pore template and nickel precursor
Mesoporous templated NiOx films were deposited onto cleaned substrates (Ti, Si) via
dipcoating performed at 25 °C and 40 % r.h. with 200 mm/min withdrawal rate. Dipcoating
solutions contained a polymer template poly(ethylene oxide)-b-poly(butadiene)-b-
poly(ethylene oxide) (PEO213-PB184-PEO213),[65, 98] 0.2 mL water (milliQ) and 2.8 mL ethanol,
to which 144.1 mg of citric acid and 436.0 mg of Ni(NO3)2·6 H2O had been added. Freshly
coated samples were dried for 10 minutes and further heat treated in air for (i) 1 hour at
250 °C and (ii) 1 hour at either 350, 400, 450 or 500 °C in a preheated muffle furnace (see
experimental part for further details).
The synthesis method relies on the thermal transformation of the deposited mesophase of
precursor complex and template polymer into the mesoporous carbonate and subsequent
conversion into nickel oxide. Thermogravimetric analysis (TGA) was therefore employed to
identify appropriate calcination conditions. Figure 14 shows the mass loss of a) template
polymer PEO-PB-PEO and b) precursor complex formed from nickel nitrate and citric acid
upon heating in air.
39
Figure 14: Thermogravimetric analysis (TGA) of a) template polymer PEO213-PB184-PEO213 and b) precursor
complex formed from nickel nitrate and citric acid. a) Polymer starts to decompose at ca. 250 °C and
rapidly decomposes between 350 °C and 425 °C. Nickel precursor complex shows a mass loss between
140 °C and 240 °C accompanied by release of CO2 (online-MS), indicating the formation of NiCO3. No
significant mass loss is observed in the range between 240 and 325 °C, indicating the presence of a
stable intermediate. Another rapid mass loss accompanied by the release of CO2 occurs for temperatures
above 325 °C, suggesting the transformation of NiCO3 to NiO.
Thermal degradation of the pore template during calcination is a commonly observed and
desirable feature of EISA based syntheses. The employed block copolymer PEO213-PB184-
PEO213 starts to decompose at temperatures around ~250 °C and rapidly decomposes
between 350 °C and 425 °C (Figure 14 a), indicating a better thermal stability than common
Pluronic type polymers.[127] The observed thermal stability of PEO-PB-PEO is similar to the
stability of poly(ethylene-co-butylene)-b-poly(ethylene oxide) (KLE), which is well-known for
its templating capabilities.[128]
The chemical complex consisting of Ni(NO3)2·6H2O and citric acid shows a distinctly different
thermal behaviour. A first mass loss occurs between 140 and 240 °C (Figure 14 b)
accompanied by release of CO2 as detected by online MS. In analogy to similar observation
reported for citric acid complexes of other metal nitrates [103, 119] the mass loss is interpreted
as a decomposition of the precursor complex into nickel carbonate.
The sample mass then remains constant between 240 °C and 325 °C indicating the presence
of a stable intermediate, i.e. nickel carbonate (Figure 14 b). Above 325 °C another rapid
mass loss of 25 % accompanied by CO2 release is observed. The formation of CO2 along
with the mass loss suggest in analogy to other systems [103, 119] that NiCO3 converts into
nickel oxide above 325 °C. Based on the obtained information, temperatures of (i) 250 °C
and (ii) 350 °C were selected to synthesize nickel carbonate and porous nickel oxide
samples for further analysis as presented in the next section.
100 200 300 400 500
0
25
50
75
100
25
50
75
100
a) Template
PEO-PB-PEO
mass / %
(i) 250 °C (ii) 350 °C
b) Complex
Ni(NO3)2+
citric acid
Template decomposition
Precursor
complex
NiCO
3
NiO
Temperature / °C
40
4.1.2 Physicochemical properties of coatings calcined at 250 °C and at 350 °C
Deposited Ni-based films calcined (i) for one hour at 250 °C and (ii) for one hour at 250 °C
and one more hour at 350 °C were investigated with respect to sample morphology,
crystalline phases and surface composition. Figure 15 presents results of the analysis by
scanning electron microscopy (SEM), transmission electron microscopy (TEM), small angle
X-ray scattering (SAXS) and selected area electron diffraction (SAED). Figure 16 displays
corresponding data obtained by a) X-ray diffraction analysis (XRD) and b) surface
composition from X-ray photoelectron spectroscopy (XPS).
Figure 15: Analysis of samples heat treated (i) for 1 h at 250 °C and (ii) for another hour at 350 °C by SEM
(a, f), TEM (b, g), SAXS at beam incident angles relative to the substrate of 90° (c, h) and 20° (d, i) as well
as SAED (e, j). Samples heat treated at 250 °C show complete penetration with templated mesopores
throughout the whole film volume (a, b) locally ordered parallel (c) and perpendicular (d) to the substrate
surface. SAED does not provide evidence for crystalline phase (e). Samples (ii) calcined at 350 °C
possess templated mesopores throughout the whole film volume (f, g) locally ordered parallel ((h) and
perpendicular (i) relative to the substrate orientation. SAXS obtained at 20 ° show a less defined pattern
indicating the onset of partial degradation of the ordered mesoporosity (i). SAED indicates crystallization
of the material into a NiO phase with rock salt structure (PDF: 00-047-1049).
Morphology. SEM images recorded for the cross section of sample (i) calcined at 250 °C
indicate the presence of mesopores in the materials cross section (Figure 15 a). The
abundant presence of mesopores throughout the bulk of the material is confirmed by TEM
images (Figure 15 b). SAXS recorded perpendicular to the substrate produces circular
diffraction patterns (Figure 15 c, β = 90°) indicative of local pore order with a d-spacing of
27.0 nm in the in-plane direction. Additional SAXS recorded at smaller angles relative to the
substrate (β = 20°) show an elliptically formed diffraction pattern with d-spacings
corresponding to 27.0 nm (in-plane) and 9.5 nm (out-of-plane, Figure 15 d). Such small-angle
diffraction patterns are typically observed for metal oxide films synthesized via EISA. The
elliptical rings can be attributed to a uniaxial and homogeneous shrinkage of film and their
100 nm 2 nm-1
100 nm
(111)
(200)
(220)
(311)
(222)
NiO
(PDF: 00 -047-104 9)
2 nm-1
SAXS 90°SEM TEM SAEDSAXS 20°
h)
c)
i)
d)
f)
a)
g)
b)
j)
e)
40 nm
40 nm
(i) 250°C
(ii) 350°C
41
mesostructure in the direction perpendicular to the substrate during calcination,[98, 104, 129]
whereas no shrinkage occurs in the in-plane direction.
SAED patterns recorded for material (i) do not show any diffraction rings or spots, suggesting
the absence of crystalline phases (Figure 15 e). This observation is consistent with the
presence of an amorphous carbonate phase as previously observed for other metal oxides
and carbonates synthesized by a similar route.[103, 119]
Samples calcined by procedure (ii) for one hour at 250 °C and subsequently for one more
hour at 350 °C were analyzed in a similar fashion (Figure 15 f-j). SEM images recorded in
top-view mode show that the complete surface of the material is penetrated by mesopores
with a pore diameter of ca. 13.7 nm (Figure 15 f). The porosity extends throughout the
complete volume of the film (TEM, Figure 15 g). SAXS patterns recorded at β=90° still show
a circular shape with a d-spacing of 26.3 nm, which is almost identical to sample (i). Also the
SAXS patterns recorded at β=20° look similar to sample (i) with d-spacings corresponding to
26.3 nm (in-plane) and 6.8 nm (out-of-plane). The decrease from 9.5 nm (250 °C) to 6.8 nm
(350 °C) indicates further shrinkage of the film in the direction perpendicular to the substrate.
The less defined pattern of the ellipse (Figure 15 i) suggests also the onset of partial
degradation of the ordered mesopore system due to calcination at 350 °C. At the same time
SAED begins to evidence a crystalline phase (Figure 15 j). All of the observed diffraction
rings can be assigned to a Nickel(II) oxide with rock-salt structure (PDF: 00-047-1049). The
data suggest that an amorphous nickel carbonate formed during calcination (i) at 250 °C is
transformed into mesoporous nickel oxide during subsequent calcination (ii) at 350 °C.
Composition. Further evidence for this transformation can be obtained from analysis of the
bulk composition (XRD, Figure 16 a) and surface composition (XPS, Figure 16 b) of the Ni
containing films deposited on Si wafers.
42
Figure 16: Influence of calcination temperature on a) crystallinity and b) surface species. a) Samples
calcined at (i) 250 °C show no evidence for crystallinity, whereas a subsequent calcination (ii) at 350 °C
leads to appearance of signals at 37.5° and 43.0°, which can be attributed to (111) and (200) reflections of
crystalline NiO in rock salt structure (PDF: 00-047-1049) with crystallite sizes of ca. 5-6 nm (Debye-
Scherrer). The crystallite size increases from 6 to 11 to 17 to 27 nm (for 111 reflection) as a function of
calcination temperature. b) XPS shows a clear signal at a binding energy of 855.7 eV for samples (i)
calcined at 250 °C, which is assigned to NiCO3. Subsequent calcination at (ii) 350 °C results in a signal at
a binding energy of 855.7 eV as well as 854.4 eV. The signal at 854.4 eV is assigned to NiO, whereas the
signal at 855.7 eV is either related to surface NiCO3 or Ni(OH)2 .
X-ray diffraction confirms that calcination (i) at 250 °C does not result in crystalline phases
(Figure 16 a, i). Samples calcined at 350 °C show clear diffraction signals at positions of 2θ
equal to 37.5° (111) and 43.0° (200), which can be assigned to crystalline NiO with rock salt
structure (PDF: 00-047-1049, Figure 16 a, ii). Applying the Debye-Scherrer equation to the
(111) and (200) reflection reveals crystallite sizes of ca. 6 nm and 5 nm, respectively. The
crystallites grow further with increasing calcination temperature up to about 27 nm for
calcination at 500 °C. X-ray diffraction analysis thus supports the interpretation of initial
formation of an amorphous nickel carbonate and its subsequent transformation into
crystalline nickel oxide.
The surface composition of samples was analysed by XPS in the Ni 2p region (Figure 16 b).
Sample (i) calcined at 250 °C show one clear signal at a binding energy of 855.7 eV. Further
heating to 350 °C results in a spectrum that can be deconvoluted into two signals with
binding energies of 855.7 eV and 854.4 eV, respectively. The signal at 854.4 eV arising at
350 °C can be assigned to NiO[130] , which is consistent with results from XRD and SAED
analysis. Unfortunately, interpretation of the signal at 855.7 eV is complicated by the fact that
two different Ni species can contribute at this binding energy, i.e. NiCO3[131] and Ni(OH)2-
870 865 860 855 850
Intensity / a.u.
Binding Energy / eV
NiO
Ni(OH)2
b) XPS (Ni 2p3/2)
NiCO3
(i) 250 °C
(ii) 350 °C
30 35 40 45 50
Intensity / a.u.
2Θ / °
a) XRD
NiO (111) (200)
(i) 250 °C
(ii) 350 °C
400 °C
450 °C
500 °C
450 °C
500 °C
43
phase.[132] However, TGA (Figure 14) indicated the presence of a carbonate bulk phase up to
325 °C and the decomposition of the nickel carbonate accompanied by a mass loss and
release of CO2 at higher temperatures. It is therefore likely, that for sample (i) calcined at
250 °C the signal at 855.7 eV corresponds to NiCO3. For sample (ii) calcined at 350 °C, the
signal at 855.7 eV could be interpreted either as a surface carbonate or nickel hydroxide.
However, the fact that the carbonate decomposes already at 325 °C makes the assignment
to a surface hydroxide more likely. A further increase in calcination temperature to 450 and
500 °C show similar curves as for 350 °C but provide less pronounced signals at binding
energies of 855.7 eV (Ni(OH)2). The decrease in intensity is possibly related to a lower
content of Ni(OH)2 within NiO obtained for as prepared samples that were heat treated at
higher temperatures.
The combined data therefore suggest that calcination (i) of the deposited films at 250 °C
forms an amorphous Nickel carbonate phase structured by the locally ordered micelles.
Further calcination (ii) at 350 °C and above transforms this phase into crystalline nickel oxide
with templated mesopore structure. The content of Ni(OH)2 in NiO of as prepared samples
seems to lower as a function of calcination temperature. The specific surface area of the
Nickel oxide corresponds to approximately 300 m2/g as derived from Kr Physisorption
(surface area) and ICP-OES (mass).
4.1.3 OER activity vs. catalyst surface area
The OER activity of NiOx samples calcined at different temperatures was studied under
alkaline conditions and compared with the surface area of the respective catalysts as
obtained from Kr-physisorption experiments. Samples were calcined for 1 h at 250 °C
followed by 1 h at either 250, 350, 400, 450 or 500 °C to obtain NiOx with different crystallinity
and surface area. OER activity was assessed by cyclic voltammetric RDE measurements in
0.1 M KOH. Figure 17 presents a) the recorded cyclic voltammograms, b) pre-oxidation
waves prior to OER onset, c) the influence of calcination temperature on the OER current
density recorded at a potential of 1.85 VRHE and d) the influence of calcination temperature on
the surface area as derived from Kr-physisorption data in m² of film per m² of the substrates
planar dimensions.
44
Figure 17: Influence of calcination temperature of mesoporous templated NiO and NiCO3 on a) OER cyclic
voltammograms, b) pre-oxidation waves c) OER current density and d) BET surface area in m² of film per
m² of the substrates planar dimensions. OER activity was assessed in a RDE setup (n=1600 rpm) in
0.1 M KOH electrolyte sweeping the potential between 1.20 - 1.95 VRHE at a scan rate of 6 mV/s. a) All
catalysts are active in OER. b) Samples heat treated at 350 and 400 °C show weak pre-oxidation
characteristics prior OER onset, usually assigned to the reversible reactions of NiO to NiOOH and Ni(OH)2
to NiOOH. c) Geometric current density compared at 1.85 VRHE as a function of calcination temperature
reveals a drastic increase in OER activity when going from 250 to 300 °C, whereas higher calcination
temperature lead to continuous decrease of OER activity. This trend in OER activity closely correlates
with d) BET surface area presented in m2 film surface per m2 substrate. The correlation suggests that the
accessible surface is one of the most important activity determining parameters.
All catalysts show significant OER currents (Figure 17 a). However, the applied calcination
temperature has a severe influence on the achieved catalytic performance. Catalytic activity
drastically increases when going from 250 to 350 °C, whereas higher calcination
temperatures of 400, 450 and 500 °C lead to continuous decrease in activity (Figure 17 c).
The highest geometric current density is reached by the sample calcined at 350 °C with
4.3 mA/cm² observed at a potential of 1.85 VRHE.
Also the shape of the recorded CVs change with calcination temperature. The most active
films, i.e. samples calcined at 350 °C and at 400 °C, show a distinct oxidation wave at about
1.50 VRHE prior to the onset of the OER (Figure 17 b). This wave is not evident for samples
calcined at temperatures of 250, 450 and 500 °C. The signals can be assigned to the
following possible electrochemical reactions. [133]
1.3 1.4 1.5 1.6 1.7 1.8
0.0
0.1
0.2
0.3
0.4
0.5
j / mA cm
-2
geo
E vs. RHE / V
a) OER activity (3
rd
CV)
1.4 1.6 1.8 2.0
0
1
2
3
4
5
6
7
j / mA cm-2
geo
E vs. RHE / V
500 °C
350 °C
450 °C
250 °C
400 °C
500 °C
350 °C 450 °C
250 °C
400 °C
b) pre-oxidation waves
250 300 350 400 450 500
0
1
2
3
4
5
6
7
j at 1.85 V vs. RHE / mA cm-2
geo
Tcalc. / °C
c) OER activity vs. T
calc.
d) BET surface area vs. T
calc.
250 300 350 400 450 500
0
5
10
15
20
25
30
35
40
45
50
BET surface area / m2m-2
Tcalc. / °C
pre-oxidation
wave
45
NiO + OH- - e- NiOOH
Ni(OH)2 + OH- - e- NiOOH + H2O
The impact of calcination temperature on the surface area of NiOx films is presented in Figure
17 d in terms of m2 of internal pore surface area of NiOx film per m2 of geometric surface area
of the planar substrate. Films calcined at 250 °C possess a very low surface area, suggesting
that this temperature is not sufficient to remove the template polymer. Calcination at 350 °C
produces the highest specific surface area, with a continuous decline at further increased
calcination temperatures. This trend in surface area as a function of calcination temperature
follows very closely the OER activity trend shown in Figure 17 c. It can be concluded that
within the range of studied synthesis parameters the accessible surface area has a
dominating impact on the resulting OER performance.
4.1.4 Electrochemical activation treatment
The overpotential observed in the present study in 1.0 M KOH at 1 mA/cm2 amounts to about
425 mV. This value is ca. 150 mV higher than the best reported Ni based catalysts based on
e.g. nanoparticle immobilization[26, 134] or nickel nitrate decomposition.[27] The lower
performance could be related to the fact that the synthesis in its present form produces
crystalline nickel oxide instead of the more active oxyhydroxides or hydroxides. According to
literature NiO is less active in the OER than nickel hydroxides or oxyhydroxides. However,
different reports suggest that nickel oxide can be transformed into a more active hydroxide
species by prolonged electrochemical treatments.[27, 135] Trotochaud et al.[27] performed a
galvanostatically anodic treatment of NiO at current densities of 10 mA/cm². After every hour
a CV was recorded to assess the resulting OER activity. The anodic treatment resulted in an
increase in OER activity from 0.2 mA/cm² to 1.0 mA/cm² (at 1.51 VRHE) after 6 hours of
treatment. Moreover, with extended treatments also the pre-oxidation wave at 1.40 VRHE
became more pronounced. Trotochaud[27] attributed the pre-oxidation/reduction wave to a
redox process of Ni(OH)2/NiOOH. The increased OER activity was rationalized by the better
ability of Ni(OH)2/NiOOH to intercalate water and anions. Furthermore, Klaus et al.[29]
reported in-situ Raman studies on electrodeposited Ni(OH)2. They observed a clear Raman
signal shift in the same potential region as the pre-oxidation waves reported by Trotochaud et
al.[27]. The Raman signals were assigned to Ni(OH)2 at lower potentials and NiOOH at higher
potentials, providing further evidence for a potential dependent transformation of Ni(OH)2 to
NiOOH.
46
We performed for the mesoporous NiO catalyst calcined at 350 °C a similar electrochemical
treatment as reported by Trotochaud et al. in order to increase the OER activity. The
treatment was performed with mesoporous templated NiO coated on titanium substrates with
5 mm in diameter and consisted of repeated potentiostatic treatments in 1.0 M KOH
(n=1600 rpm) at a potential of 1.75 VRHE for 5 hours. After every hour of potentiostatic
treatment an intermediate CV was recorded in the OER range by sweeping the potential with
20 mV/s from 1.75 VRHE to 1.20 VRHE and back to 1.75 VRHE in order to assess OER
performance as well as pre-oxidation and corresponding reduction waves. Alternating
potentiostatic treatments and CV measurement were repeated 5 times to follow the catalyst
activation. In order to assess also the subsequent OER activity 20 consecutive CVs in the
OER region were performed after 10 hours of potentiostatic treatment at 1.75 VRHE. Figure 18
displays a, b) the CVs recorded initially as well as after 1, 3 and 5 h of potentiostatic
treatment, c) the OER-related current density observed at 1.70 VRHE during the CV sweeps
and d) the 2nd, 5th, 10th and 20th CV after 10 hours of potentiostatic treatment.
Figure 18: Influence of potentiostatic activation treatment at 1.75 VRHE for NiO calcined at 350 °C on a,b)
CV shape and c) OER activity. Subsequent OER performance of modified NiO is investigated with d) 20
consecutive CVs after 10 hours of potentiostatic treatment. a, b) CVs in the OER range recorded with a
sweep rate of 20 mV/s from 1.75 VRHE to 1.20 VRHE before and after several electrochemical potentiostatic
treatments at a potential of 1.75 VRHE for 1 hour each. With each treatment OER activity increases (a) and
the pre-oxidation wave at 1.47 VRHE as well as the corresponding reduction wave at 1.28 VRHE become
more pronounced (b). c) Quantification of the activation in terms of observed geometric current density at
1.7 VRHE after repeated activation treatments. d) OER performance is further enhanced also by conducting
another 20 consecutive CVs after 10 hours of potentiostatic activation treatment.
1.2 1.4 1.6 1.8 2.0
0
1
2
3
4
5
6
7
8
j / mA cm
-2
geo
E vs. RHE / V
initial
after 1 h
after 3 h
after 5 h
iR corrected,
1.0 M KOH
a) CVs recorded after different
duration of activation
c) geometric OER current densities
compared at 1.7 V vs. RHE
0 1 2 3 4 5 6
0
1
2
3
4
5
6
7
8
j at 1.7 V vs. RHE
(anodic) / mA cm-2
geo
Duration of potentiostatic treatment / h
d) subsequent CVs in
the OER range
1.2 1.3 1.4 1.5 1.6 1.7 1.8 1.9 2.0
0
1
2
3
4
5
6
7
8
j / mA cm
-2
geo
E vs. RHE / V
iR corrected,
1.0 M KOH
CV2
CV5
CV20
CV10
b) magnification of CVs
prior OER onset
1.2 1.3 1.4 1.5 1.6
-0.4
-0.2
0.0
0.2
0.4
0.6
0.8
j / mA cm
-2
geo
E vs. RHE / V
initial
after 1 h
after 3 h
after 5 h
47
The potentiostatic treatment resulted in two major changes of the catalyst’s electrochemical
behaviour. With each hour of treatment the pre-oxidation wave observed at about 1.47 VRHE
and the corresponding reduction wave at 1.28 VRHE became more pronounced (Figure 18 b),
indicating an improved redox ability. Moreover, also the current density observed in each
subsequent CV became higher, indicating an increased OER performance (Figure 18 a).
Figure 18 c shows a quantitative evaluation of the increased activity by showing CVs
conducted between 1 and 5 h of potentiostatic treatment. The OER-related current density
obtained at a potential of 1.70 VRHE steadily increases from initially 2.7 mA/cm² to about
4.0 mA/cm² after 5 h of potentiostatic treatment. Figure 18 d depicts the OER activity during
subsequent repeated CVs. The measured OER activity at 1.70 VRHE further increases up to
5.1 mA/cm² accompanied by a small increase of the pre-oxidation wave, indicating the
opportunity for a further enhancement of OER activity. Both observed effects, the increase in
pre-oxidation wave currents as well as the increased OER activity, are in full agreement with
the report of Trotochaud et al.[27] It can be concluded, that the activity of the synthesized
mesoporous nickel oxide can be further increased by extended anodic treatments that
convert parts of the near-surface region of the catalyst into Ni(OH)2 or NiOOH
4.1.5 OER activity comparison with reported catalysts
The overpotential is often used as a measure of catalytic activity and was quantified for the
most active catalysts at 1 mA/cm² planar geometrical current density. The derived
overpotential is then related to values obtained in previous studies reported in literature.
Yu et al.[23] prepared a nickel-based thin film (NiOx) on multi walled carbon nanotubes
deposited on ITO and observed an OER overpotential of 523 mV. Singh et al.[24]
electrodeposited layers of nickel oxide from [Ni(en)3]Cl2 (en= 1,2-diaminoethane) on glassy
carbon and reported 510 mV overpotential. Nardi et al.[25] deposited thin films of NiO Ni(Cp)2
(cp=cyclopentadienyl) on fluorine doped tin oxide (FTO) via atomic layer deposition and
achieved an overpotential of 400 mV. Lyons et al.[37] investigated the electrocatalytic activity
of polycrystalline nickel foils and reported an overpotential of 379 mV. Fominykh et al.[26]
prepared NiO nanoparticles using a solvothermal reaction in tert-butanol. Subsequently, NiO
nanoparticles were deposited on Au-coated QCM electrodes in order to access the OER
overpotential (280 mV). Trotochaud et al.[27] obtained a thin film of NiOx by spincoating a
solution containing Ni(NO3)2·6H2O on Au-coated QCM electrodes. Subsequent
electrocatalytic investigation in the OER regime revealed an overpotential of 279 mV.
Figure 19 shows reported overpotentials for nickel based catalysts at 1 mA/cm² and
corresponding electron micrographs.
48
Figure 19: Comparison of OER overpotentials at 1 mA/cm² for mesoporous templated NiO (red columns)
with previous reported literature data (black columns), and electron micrographs of the corresponding
samples. The observed overpotential for mesoporous templated films of NiO (350 °C) decreases from
425 mV to 383 mV after 5 h of potentiostatic treatment. Subsequent CVs recorded after 10 h of
potentiostatic treatment result in further decrease of the observed overpotential (369 mV).
The literature reports for different nickel based catalysts show OER overpotentials in the
range between 523 mV and 279 mV to achieve a geometrical current density of 1 mA/cm².
PEO-PB-PEO templated films of NiO calcined at 350 °C subsequently treated by an
electrochemical activation procedure (chapter 4.1.4) show a fairly high OER overpotential of
369 mV. The observed overpotential is ca. 90 mV higher than the best reported Ni based
catalysts based nanoparticle immobilization[26] or nickel nitrate decomposition.[27] The
depicted lower activity could be related to the fact that the synthesis in its present form
produces crystalline nickel oxide and that a total conversion to the more active oxyhydroxides
or hydroxides by electrochemical treatment was not achieved. However, OER overpotentials
reported by Fominykh et al. (280 mV)[26] and Trotochaud et al. (279 mV)[27] were both tested
for nickel oxide based catalysts deposited on gold substrate. According to Pourbaix[136] the
thermodynamic equilibrium potential of the Au/Au+III redox couple is found to be 1.50 VRHE.
The observed OER overpotentials for nickel oxide catalysts on gold (1.51 VRHE) and the
thermodynamic equilibrium potential of the Au/Au+III redox couple (1.50 VRHE) are so close to
0
100
200
300
400
500
600
Overpotential at 1 mA cm
-2
geo
/ mV
initial
1
st
CV (after 5 h)
20
th
CV (after 10 h)
-42 mV -14 mV
NiO
x
electrodepo-
sitedon MWCNT-ITO
Yu et al.
ACS Appl. Mater.
Interfaces, 2014
6, 15395-15402
NiO
x
electro-
deposited on GC
Singh et al.
Energy Environ. Sci.
2013, 6, 579-586
NiO ALD on FTO
Nardi et al.
Adv. Energy Mater.
2015, 5, 1500412
OxidizedNickel-
electrode
No image
published
Lyons et al.
J. Electroanal. Chem.
2010, 641, 119-130
Fominykh et al.
Adv. Funct. Mater.
2014, 24, 3123-3129
NiO NP on Au
100 nm
NiO
x
film on Au
Trotochaud et al.
J. Am. Chem. Soc.
2012, 134, 17253-17261
49
each other that the observed higher activity of such catalysts is probably attributed to
oxidation of gold rather than oxygen evolution.
In summary it is shown that for the first time NiO films with ordered mesopore structure can
be synthesized via soft-templating and proof to be active in OER catalysis. The synthesis
succeeds by employing a metal complex formed from citric acid and nickel nitrate along with
a polymer template PEO213-PB184-PEO213 to perform deposition via evaporation-induced self
assembly. Calcination at 250 °C converts the deposited film into an amorphous carbonate,
whereas higher calcination temperatures transform the carbonate into NiO while retaining the
templated mesopore structure. All catalysts obtained by this synthesis possess significant
OER activity, with samples calcined at 350 °C exhibiting the highest OER performance and
the highest surface area. A further increase in OER activity for mesoporous NiO layers can
be achieved by potentiostatic treatments at 1.75 VRHE. This observation is in line with reports
in literature[27] and is explained by an in-situ transformation from NiO to Ni(OH)2/NiOOH,[29]
assuming that NiOOH is most likely the active phase for OER.
Chapter 4.1 focused solely on oxides of one metal only, i.e Ni. Since mixed metal oxides of
Ni with e.g. Fe, Co were reported to show higher intrinsic activities than nickel oxide, a further
increase in OER performance can probably be achieved if the synthesis of corresponding
mixed metal oxide film with micelle-controlled mesopore structure succeeds. However, the
next chapter illustrates the synthesis pathway for the production of highly active OER
catalysts operating under acidic conditions.
50
4.2 Mesoporous templated IrO2 synthesized from Ir(OAc)3
Electrolysers operating in acidic media provide several advantages compared to
electrolysers in alkaline media, such as high current density (> 2 A/cm²), lower gas crossover
rate, lower operational costs and high pressure output (also see chapter 2.1 for detailed
description). Typical electrolysers are limited by the OER due to the fact that four electrons
are needed to produce one molecule of oxygen and that the OER proceeds by a complex
reaction mechanism.[13, 45-46] Electrocatalytic water splitting performed in acidic media
therefore appears to be an attractive approach for a more efficient generation of molecular
hydrogen. A major roadblock is to find materials that withstand corrosive conditions and
provide significant electron conductivity. The oxides of ruthenium and iridium show the lowest
OER overpotential in acidic media.[13, 52-53] Although ruthenium oxide shows higher activity, it
typically corrodes during OER potential cycles. iridium oxide is therefore the best
compromise for an active and stable OER catalyst.[13] However, limited abundance and
competition with applications such as supercapacitors,[66-67] stimulating neural electrodes[68-69]
and microelectrodes for pH sensing[70-71] require the most efficient utilization of IrO2 that is
possible.
Chapter 4.2 presents the potential of pore templating with polymer micelles in order to
produce model-type porous catalysts for the investigation of structure-activity relationships in
gas evolution reactions and for the optimization of the performance of IrO2-based OER
catalysts. The presented synthesis approach is based on pore templating with micelles of
amphiphilic block copolymers PEO-PB-PEO (chapter 4.2.1) and further improved to produce
iridium oxide films with controlled pore size, film thickness and crystallinity (chapter 4.2.2).
The model systems are used to study the influence of porosity and crystallinity on
electrochemically accessible surface area (ECSA), OER performance, gas transport and
faradaic efficiency (chapters 4.2.3 - 4.2.4). A controlled variation in thickness of the porous
catalysts explores, which parts of the catalyst can be utilized without transport limitations
during high-current OER (chapter 4.2.5). The combined knowledge is used to design a
multilayer-IrO2 catalyst that shows the lowest OER overpotential reported so far for
monometallic oxide compounds of Ir.
51
4.2.1 Physicochemical properties of PEO-PB-PEO templated mesoporous IrO2
A dipcoating solution was prepared by dissolving PEO-b-PB-b-PEO triblockcopolymer and
Ir(OAc)3 in ethanol. Subsequently, dipcoating was performed on silicon substrate at a
temperature of 25 °C and a relative humidity of 40 %. The as synthesized films were
thermally treated at 375 °C in a preheated muffle furnace under air atmosphere. The
obtained layers were physicochemical characterized in order to investigate morphology, layer
thickness, crystallinity and locally pore ordering.
Figure 20 shows for mesoporous templated IrO2 a) SEM, b) cross section SEM, c) TEM, d)
SAED, SAXS at e) 90° and f) 20° with respect to the film surface normal and g) Kr-
physisorption.
Figure 20: Physicochemical properties of mesoporous PEO-PB-PEO templated IrO2 dipcoated on silicon
wafers and subsequently heat treated under air atmosphere. All samples were calcined at 375 °C, except
for samples investigated by SAXS (400 °C). a) Templated mesoporosity is visible on the outer surface
plane area. b) Layer thickness was revealed by cross section SEM and amounts to 103 nm. c) TEM
micrographs were recorded from samples scratched off from silicon substrate and subsequently
deposited on a TEM grid. d) Selected area electron diffraction images were recorded for investigating
crystallinity. Pore ordering was determined by SAXS with an incident beam e) parallel (90°) and d)
perpendicular (20°) to the film normal. g) BET surface area derived by Kr-physisorption is presented in m2
film surface per m2 substrate.
SEM images were recorded in top view mode in order to provide information about the
morphology of the outer surface plane area. Figure 20 a shows a PEO-PB-PEO templated
film calcined at 375 °C exhibiting pores that are uniform in shape and size. The diameter of
the mesopores amounts to 21±4 nm. The corresponding FFT of the top view SEM image
(inset Figure 20 a) shows an isotropic ring revealing the presence of an ordered pore
a) SEM b) cross section SEM c) TEM
g) Kr-physisorptione) SAXS 90°f) SAXS 20°
d) SAED
400 °C 400 °C
(101)
(110)
77 m² m-²
103 nm
100 nm 20 nm 2 1/nm
(321)
(220)
(211)
52
arrangement at the outer surface plane area with a periodic pore distance of 18 nm. The
observed pore walls show a thickness of 11±1 nm as well as additional pores that appear to
be smaller than 2 nm in size. The textural porosity is also present for untemplated samples[65]
indicating that the presence of the template polymer does not introduce textural porosity. A
possible explanation for that behaviour would be the formation of CO2 during thermal
decomposition of the acetate precursor.
The layer thickness was investigated by breaking a substrate coated with a mesoporous
layer of IrO2 into half and viewing it from the side by SEM. Figure 20 b presents for a sample
heat treated at 375 °C a SEM micrograph recorded in cross section mode. The layer
thickness amounts to 103 nm which is a typical value reported in literature for similar
synthesized IrO2. (ca. 100 nm - 150 nm)[65]
Figure 20 c depicts TEM micrographs revealing spherical mesopores with a diameter of ca.
20 nm, indicating that pores penetrate the sample throughout the whole film volume area.
The local crystallinity of mesopore walls was studied by electron diffraction analysis on IrO2
samples removed from substrate and placed on TEM grids. Figure 20 d shows SAED
measurements of for a sample calcined at 375 °C. The sample shows very broad diffraction
rings, indicating the onset of crystallization. The observed diffraction rings correspond with
the lattice parameters of crystalline IrO2 rutile (PDF 150870). The presence of broad
reflection rings lead to the assumption that the synthesis produces films with small
crystallites.
Insight of pore ordering is granted by SAXS and is shown for samples heat treated at 400 °C
with the silicon substrate positioned perpendicular and parallel to the incident beam.
Measurements with the substrate in transmission mode (90 °, Figure 20 e) display isotropic
rings indicating well ordered porosity parallel to the substrate, whereas the out-of-plane
measurement (10°, Figure 20 f) shows an elliptically distorted ring, indicating contraction of
the pore system perpendicular to the substrate.
The surface area of layers coated on silicon substrate was investigated with krypton
physisorption and is shown in Figure 20 g. The calculated BET surface area amounts to
91 m² film surface area per m² substrate geometric surface area indicating that most of the
containing polymer template was removed and that an accessible mesopore system is
produced. The surface area is in good agreement with reports in literature for mesoporous
templated IrO2 thermally treated at 400 °C (130 m²/m²).[65]
The combined physicochemical techniques thus suggest that the synthesis in its present
form successfully introduces an accessible (Figure 20 g) open mesoporous system (Figure
20 a, c) into a metal oxide with low crystallinity (Figure 20 d). The established mesoporosity
appears locally ordered parallel and perpendicular (Figure 20 e, f) to the film surface normal.
53
4.2.2 Influence of calcination temperature on morphology, ECSA and OER
The calcination temperature of micelle-templated oxide films can strongly influence the
precursor decomposition, template removal and the obtained film morphology and surface
area.[65] In order to relate the morphology of templated iridium oxide to its accessible surface
area and catalytic activity dip-coated films were calcined at temperatures of 325, 350, 375,
400, 475, 550 and 625 °C and analyzed by SEM, ECSA measurements and OER testing.
Figure 21 presents for selected calcination temperatures (a) top-view SEM images, (b) CVs
in the ECSA range[55, 125-126] and (c) CVs recorded in the OER potential range.
Figure 21: Influence of calcination temperature of micelle-templated iridium oxide films on a) film
morphology, b) electrochemically accessible surface area and c) OER performance. a) top-view SEM
images, b) CVs recorded in the ECSA range between 0.40 and 1.40 VRHE at 50 mV/s and c) CVs recorded in
the OER range between 1.20 and 1.65 VRHE at 6 mV/s. All samples were coated on Ti cylinders and
calcined for 5 min at the indicated temperature. All electrocatalytic data were recorded in 0.5 M H2SO4
electrolyte with rotating working electrode, RHE reference and Pt gauze counter electrode.
SEM images of the sample calcined at 325 °C (Figure 21 a - 325 °C) show charging, which
indicates that the polymer template is not fully removed at this temperature and still blocks
a) SEM
100nm
100nm
100nm 100nm 100nm 100nm 100nm
T
calc.
= 325 °C 350 °C 375 °C 400 °C 475 °C 550 °C 625 °C
0.4 0.6 0.8 1.0 1.2 1.4 1.6
-2.5
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
2.5
j / mA cm-2
geo
E vs. RHE / V
0.4 0.6 0.8 1.0 1.2 1.4 1.6
E vs. RHE / V
325 °C
350 °C
375 °C
400 °C
475 °C
550 °C
625 °C
400 °C
475 °C
550 °C
625 °C
1.2 1.3 1.4 1.5 1.6 1.7
E vs. RHE / V
1.2 1.3 1.4 1.5 1.6 1.7
0
20
40
60
80
100
j / mA cm
-2
geo
E vs. RHE / V
325 °C
350 °C
375 °C
c) OER
b) ECSA
2nd cycle, iR corrected 2nd cycle, iR corrected
2nd cycle, iR corrected 2nd cycle, iR corrected
54
the pore system. Films treated at higher temperatures of 350, 375, 400 and 475 °C feature a
fully developed system of locally ordered mesopores (see e.g. SAXS data for calcination at
400 °C as presented in Figure 20 e and f) with pore diameters of ca. 21±4 nm and a wall
thickness of 11±1 nm (values derived from Figure 21 a, 350 - 475 °C). The obtained
mesoporosity agrees well with the pore morphology typically observed for oxide films
templated by micelles of the pore template PEO-PB-PEO (TiO2,[98] MgO,[103] ZnO,[119]
Co3O4[119]). Moreover, SEM images of films calcined at 550 and 625 °C indicate the beginning
deformation of the circular mesopore shape, which can be attributed to the onset of sintering.
The ECSA corresponding to each sample can be derived from the current response
(normalized to the substrate geometric surface area) in the potential range between 0.40 and
1.40 VRHE as plotted in Figure 21 b. Samples calcined at 325 °C show a very small surface
area (Figure 21 b). This observation is in good agreement with the SEM analysis where
significant charging was observed. If charging is caused by incomplete removal of the pore
template then the pore system is still blocked and not electrochemically accessible. For
samples calcined at intermediate temperatures (Figure 21 b, 350 °C, 375 °C) a rapid
increase in current density and accessible surface is observed. Temperature treatments at
400 °C and above progressively decrease the ECSA, yielding lowest ECSA values for
samples heat treated at 625 °C.
OER performance was measured on the same catalysts by CVs in the potential range of 1.20
to 1.65 VRHE. Figure 21 c shows the current response normalized to the Ti cylinders
geometrical surface area. The OER activity strongly depends on the applied calcination
temperature. All catalysts except for the sample calcined at 325 °C show significant OER
activity. The OER activity increases up to 375 °C, whereas higher calcination temperatures
lead to a progressing decrease in OER activity. Similar trends in ECSA and OER
performance are also observed under alkaline conditions (see Figure A1 a, b).
The electrocatalytic OER performance of mesoporous templated IrO2 calcined at 375 °C is
further correlated to fundamental model type catalysts, e.g. cylinders of polycrystalline[56] and
single crystalline Ir.[137] The electrocatalytic performance was investigated by cyclic
voltammetry and the current response was normalized to the substrates planar geometrical
surface area.
Figure 22 shows the OER activity measured for a bulk Ir-cylinder, an Ir(110) single crystal
and a mesoporous templated IrO2 heat treated at 375 °C.
55
Figure 22: Comparison of OER activity for mesoporous templated IrO2, Ir(110) single crystal[137] and Ir-
cylinder (bulk).[56] At a potential of 1.53 VRHE the mesoporous templated IrO2 films (375 °C) exhibit an
approximately 20 times higher current density compared to Ir(110) single crystal and Ir-cylinder.
The observed OER activity strongly depends on the utilized system. However, the Ir (110)
single crystal and the Ir-cylinder (bulk) show a very low current response in the OER potential
window, whereas mesoporous templated IrO2 calcined at 375 °C depict a significant higher
OER activity. The mesoporous catalyst calcined at 375 °C is about 20 times more active than
a single crystal Ir(110) or an Ir-cylinder (bulk).
The overpotential can be used as a measure of catalytic activity. Under standard conditions
the thermodynamic minimum potential in the OER amounts to 1.23 VRHE. Table 1 lists the
respective overpotentials recorded at a current density of 0.5 mA/cm². The lowest
overpotential (0.212 V) is observed for a sample calcined at 375 °C. Calcination at
temperatures of 475 °C and above result in significantly increased overpotential values.
Table 1 also lists overpotentials obtained by Reier et al.[64] on similarly prepared catalysts
without templated mesoporosity, which results in e.g. 32 mV and 72 mV higher overpotentials
for calcination at 350 and 550 °C, respectively. Summarizing, mesoporous templated IrO2
shows a significant higher electrocatalytic OER activity than untemplated IrO2.[64] The higher
geometrical OER activity is related to the fully accessible porous system introduced by PEO-
PB-PEO polymer template. The control in size, distance and connection of the templated
mesopores allows the design of highly active OER catalysts.
1.2 1.3 1.4 1.5 1.6
0
20
40
60
80
100
j / mA cm-2
geo
E vs. RHE / V
IrO2, 375 °C,
single layer
Ir(110)
singlecrystal
Ir-cylinder (bulk)
Comparison of OER activity
56
Table 1: Influence of calcination temperature on OER overpotential (at 0.5 mA/cm²) and comparison to
IrO2 without templated mesopores (from [64]). Mesoporous IrO2 heat-treated at 375 °C (highlighted in bold
type) show the lowest overpotential.
Applied
Tcalc. / °C
Overpotential / V at
0.5 mA cm-2
(IrO2, this work)
Overpotential / V at
0.5 mA cm-2
(untemplated IrO2
[64]
)
325
No significant activity
350
0.228
0.26
375
0.212
400
0.218
475
0.228
550
0.278
0.35
625
0.307
4.2.3 Faradaic efficiency
The production of H2O2 and dissolution of the catalyst are common side reactions of the
OER. Both effects were tested for. Titration with 0.001 mol/l KMnO4 solution was performed
on fresh electrolyte and after 50 OER cycles with the most active catalyst (Tcalc. =
375 °C) to test for H2O2. No significant differences were observed between the two
electrolytes, suggesting that negligible amounts of H2O2 were formed. Moreover, ICP-OES
analysis of the used electrolyte did not detect dissolved iridium species within the limits of
experimental accuracy. Both tests suggest a high faradaic efficiency of the IrOx catalysts.
In order to test further if residual carbon that could potentially remain after catalyst synthesis
affects the OER current, additional tests were conducted by differential electrochemical mass
spectrometry (DEMS) performed during OER while measuring the formed CO2 and O2 via
MS. The detected product gases were O2 and CO2. The observed O2 concentration for the 1st
applied CV amounts to 98.7 %, the rest being CO2.The O2 selectivity further increases to
98.8 % for the 2nd CV and 99.9 % for the 10th applied cycle (see Figure A2). Hence, the
current resulting from the removal of residual carbon during OER is rather small.
4.2.4 Relationship between OER activity, ECSA and sample crystallinity
The relation between the catalysts accessible surface area and the respective OER
performance was further analyzed by quantification of the respective electrochemical data.
Figure 23 plots as a function of calcination temperature (a) the total charge obtained by the
mean value of the integrated anodic and cathodic currents in the ECSA range as a measure
of the catalysts total surface area, (b) BET surface area presented in m2 film surface per m2
substrate (c) the current density normalized to the geometric electrode surface area recorded
at 1.55 VRHE during OER potential scans as a measure of OER activity, and (d) the current
density at 1.55 VRHE normalized to the ECSA charge as an indicator of each catalysts intrinsic
activity.
57
Figure 23: ECSA, BET surface area, OER activity and ECSA-normalized activity of mesoporous iridium
oxide as a function of calcination temperature. a) ECSA as total charge obtained as a mean value of the
integrated anodic and cathodic currents between 0.40 and 1.40 VRHE, b) BET surface area in m² film
surface normalized with respect to the substrates planar geometrical surface area c) current density
recorded at 1.55 VRHE normalized to the geometric electrode surface area, and d) geometric current
density at 1.55 VRHE normalized to the ECSA charge as an indicator of each catalysts intrinsic activity.
The ECSA increases from 325 °C to 375 °C with increasing calcination temperature (Figure
23 a) and then rapidly decreases between 400 and 625 °C. The catalysts surface area
measured by Kr physisorption shows a very similar behavior and peaks at the same
calcination temperature of 375 °C (Figure 23 b). Also the observed OER activity follows this
trend (Figure 23 c). The OER activity increases rapidly with increasing calcination
temperature reaching a maximum for 375 °C and steadily declines with further temperature
increase. Figure 23 d relates for each calcination temperature higher than 325 °C the
measured OER activity to the respective ECSA. It can be seen that this surface-area
normalized activity stays almost constant for calcination between 350 and 475 °C, but
steadily decreases for higher calcination temperatures. It is therefore evident that at least two
major factors contribute to the overall OER activity, i.e. the accessible surface area as well as
the intrinsic activity of each accessible site.
In order to relate the observed ECSA and activity trends to structural and compositional
properties of the porous IrO2 catalysts the respective samples were studied by XRD, SAED
and TEM. Figure 24 presents a) diffractograms for the catalyst calcined at different
300 350 400 450 500 550 600 650
0
1
2
3
4
5
6
7
8
ECSA / mC
T
calc
/ °C
a) ECSA
c) OER activity d) Activity / ECSA
300 350 400 450 500 550 600 650
0.0
2.0x103
4.0x103
6.0x103
8.0x103
1.0x104
1.2x104
j (at 1.55 V vs. RHE)
per ECSA /mA cm-2 C-1
Tcalc / °C
300 350 400 450 500 550 600 650
0
5
10
15
20
25
30
35
40
j at 1.55 V vs. RHE / mA cm-2
geo
Tcalc / °C
300 350 400 450 500 550 600 650
0
10
20
30
40
50
60
70
80
BEt surface area / m² m
-2
T
calc
/ °C
b) BET surface area
2nd cycle, iR corrected
58
temperatures, b) selected area electron diffraction images and c) bright-field TEM images for
representative samples calcined at 350, 375, 475, 550 and 625 °C.
Figure 24: Analysis of crystallinity (XRD, SAED) and morphology (TEM) for mesoporous iridium oxide
calcined at different temperatures between 350 and 625 °C. a) diffractograms for a polished titanium
cylinder, the Ti cylinder calcined at 550 °C and for IrOx-coated Ti-cylinders (350 – 625 °C). b) SAED
analysis for IrOx samples calcined at 350, 375, 475, 550 and 625 °C. Indexing corresponds to IrO2 rutile
(PDF 150870), c) analysis of the pore structure of the samples by TEM.
The Ti substrate shows after polishing only the expected reflections that correspond to
metallic Ti (PDF 00-044-1294) (Figure 24 a, "Ti cyl"). Heat treatment of the substrate under
typical calcination conditions of this study (5 min, 550 °C) does not lead to a measurable
formation of crystalline titanium oxides anatase or rutile (Figure 24 a, "Ti cyl 550 °C").
Coating the substrates with mesoporous iridium oxide and calcining at temperatures between
350 and 475 °C does not produce any additional reflections (Figure 24 a, 350 - 475 °C).
Hence, the corresponding catalytic layers are X-ray amorphous: IrO2 has either not
crystallized yet or crystallites are too small to provide sufficiently intense diffraction signals.
However, calcination at temperatures of either 550 °C or 625 °C result in broad reflections at
a) XRD b) SAED c) TEM
20nm
20nm
20nm
2 1/nm
625 °C
475 °C
350 °C
2 1/nm
2 1/nm
625 °C
475 °C
350 °C
(101)
(200)
(211)
(110)
(220)
(112)
(321)
(312)
(310)
350 °C
375 °C
400 °C
475 °C
550 °C
625 °C
Ti (100) (002) (101)
IrO2(110) (101) (200)
Ti cyl
550 °C
Ti cyl
25 30 35 40 45
2 Θ / °
Intensity / a.u.
375 °C
2 1/nm
375 °C
20nm
550 °C 550 °C
2 1/nm 20nm
59
2-theta positions of 28.1 and 34.7° (Figure 24 a, 550 °C, 625 °C). The signals correspond
well with the (110) and (101) reflections of crystalline IrO2. An estimate by Scherrer equation
provides a crystallite size of about 4 nm (550 °C). Increasing the calcination temperature to
625 °C increases the IrO2 crystallite size to ca. 5 nm. X-ray diffraction analysis therefore
suggests that calcination at 550 °C and higher temperatures forms crystalline IrO2, which is
absent at lower calcination temperatures.
The local crystallinity of mesopore walls was studied by electron diffraction analysis on IrO2
samples removed from the Ti substrate and placed on TEM grids. Figure 24 b presents
SAED images of samples calcined in air at 350, 375, 475, 550 and 625 °C, respectively.
Films calcined at 350 and 375 °C show very broad diffraction rings, indicating the onset of
crystallization. Samples calcined at 475 °C feature narrow diffraction rings. The respective
hkl-indices (Figure 24 b, 475 °C) correspond well with the lattice parameters of crystalline
IrO2 rutile (PDF 150870). Calcination at 550 and 625 °C produces sharp diffraction rings with
clearly distinguishable diffraction spots indicative of higher material crystallinity. SAED
analysis of film samples removed from the substrate thus confirms the phase assignment to
IrO2 rutile. Crystallinity increases with increasing calcination temperature, with significant
amounts of crystalline iridium oxide being present already at 475 °C.
TEM analysis for the same samples (Figure 24 c) confirm that calcination at 350 °C, 375 °C
and 475 °C yields spherical mesopores origination from the pore template. However, the
progressing crystallization at 550 and 625 °C leads to sintering, which results in deformation
of the initially spherical pore shape (Figure 24 c, 550 °C, 625 °C). The combined XRD, SAED
and TEM data thus suggests that catalyst films calcined between 350 and 475 °C are
composed of iridium oxide with low crystallinity, whereas calcination at 550 or 625 °C
produces a mesoporous well-crystallized IrO2 rutile phase with slightly degraded pore
structure.
Morphology and phase composition (Figure 24) can now be related to the ECSA and activity
data (Figure 23). The lowest studied calcination temperature (325 °C) is too low to
decompose template polymer. Hence pores are blocked and neither significant ECSA (Figure
23 a) nor OER activity (Figure 23 c) can be observed. Calcination at 350 °C or 375 °C
removes the template polymer and forms an iridium oxide with very low crystallinity (Figure
24 b) but highly accessible pore structure (Figure 23 a, b). The accessible pore structure
consists of highly active sites (Figure 23 c), which results in optimal OER performance
(Figure 23 b).
60
Calcination at 400 or 475 °C produces a porous iridium oxide composed of sites with similar
intrinsic activity (Figure 23 d). However, the ECSA decreases significantly with increasing
calcination temperature (Figure 23 a) resulting in lower OER performance (Figure 23 c).
A further increase in calcination temperature to 550 and 625 °C forms a well crystallized IrO2
(Figure 24 a, b) with a pore structure degraded by sintering (Figure 24 c). The sintering
results in a further decreasing ECSA (Figure 23 a). Moreover, also the activity per accessible
site decreases clearly with increasing material crystallinity (Figure 23 d). In consequence,
overall OER performance decreases even further.
The activity of pore-templated iridium oxide films is therefore determined by at least two
major factors, i.e. the accessible surface area which reaches an optimum at 375 °C, and the
intrinsic activity of the accessible sites, which is high between 350 and 475 °C. The best
overall performance is thus obtained for calcination at 375 °C.
Similar trends for the intrinsic OER activity were found by Reier et al. on untemplated iridium
oxide thin-film catalysts.[64] They observed that the intrinsic OER activity remained
independent of the calcination temperature between 250 and 350 °C, but decreased with
calcination at 450 °C and at higher temperatures. High activity was assigned to an
amorphous low temperature iridium oxide, whereas crystalline high-temperature oxide was
reported to be less active. However, they did not observe an increase in ECSA and
geometric OER activity between 325 and 375 °C suggesting that this effect is related to the
removal of the pore template.
4.2.5 Single layer and Multilayer dipcoating - Influence of withdrawal rate on layer
thickness, ECSA, OER and discussion of transport limitation
The transport of evolved gases can be limiting at high current densities. Zeradjanin et al.
[138-140] studied the influence of the catalysts structure on the detachment of gas bubbles.
Cracked surfaces, i.e. surfaces with added transport pores, showed a higher frequency of
bubble detachment in oxygen and chlorine evolution than crack-free samples. Adding
sufficiently large pores to OER catalysts could therefore provide a large and accessible
active surface area and facilitate the transport of evolved gases. Moreover, quantitative
studies of transport effects in gas evolution reactions would benefit from the availability of
catalysts with defined and tuneable pore size.
The number of potentially active sites of a homogeneous catalytic coating is expected to
scale linear with the amount of coating (i.e. film thickness) and its specific surface area. By
increasing the withdrawal rate of the Ti substrates mesoporous single-layer iridium oxide
coatings were prepared with higher film thickness in order to increase the catalysts overall
61
OER performance. However, the thickness of crack-free single layers of oxides that can be
produced by EISA is limited.[111] Therefore, thicker films were produced by a new multilayer
dipcoating procedure with intermediate calcination steps. The films were employed as
scalable model systems with defined porosity to test if the transport of electrons to the active
sites and/or the pore transport of produced oxygen gas to the outer film surface becomes
limiting for thicker films at higher current density. Figure 25 shows a) SEM cross-section
images, b) ECSA analysis and c) OER performance for the respective films.
Figure 25 a) Cross section SEM images of mesoporous iridium oxide single- and multilayer films obtained
by dipcoating. By adjusting withdrawal rate, controlled film thickness between ~50 and ~225 nm can be
achieved in single layer regime. In order to obtain thicker layers multilayer films were synthesized. b) CVs
measured in the ECSA potential region between 0.40 and 1.40 V vs. RHE. For thicker layers the current
appears to be progressively larger, hence the multi layer sample obtains the highest ECSA. c) CVs
measured in the OER range for different layer thicknesses. The OER activity increases with increasing
layer thickness. The 480 nm thick multilayer catalyst achieves the lowest overpotential (0.20 V at
1.0 mA/cm²).
Mesoporous crack-free catalyst films were obtained for all single-layer coatings up to a
withdrawal rate during dip-coating of 150 mm/min. (Note that the cracks visible in Figure 25 a
are a result of sample preparation for film thickness analysis, not of the synthesis procedure.)
The thickness of the produced mesoporous single-layer iridium oxide increases linear with
increasing withdrawal rate of the substrate from 50 nm (10 mm/min) to 120 nm (50 mm/min),
170 nm (100 mm/min) and finally 225 nm (150 mm/min). A further increase in film thickness
by faster substrate withdrawal resulted in cracking and peel-off of the films during calcination.
However, significantly thicker films (480 nm) were produced by multilayer deposition
0.4 0.6 0.8 1.0 1.2 1.4
-6
-4
-2
0
2
4
6
j / mA cm
-2
geo
E vs. RHE / V
0.4 0.6 0.8 1.0 1.2 1.4
-6
-4
-2
0
2
4
6
j / mA cm
-2
geo
E vs. RHE / V
0.4 0.6 0.8 1.0 1.2 1.4
-6
-4
-2
0
2
4
6
j / mA cm
-2
geo
E vs. RHE / V
0.4 0.6 0.8 1.0 1.2 1.4
-6
-4
-2
0
2
4
6
j / mA cm
-2
geo
E vs. RHE / V
0.4 0.6 0.8 1.0 1.2 1.4
-6
-4
-2
0
2
4
6
j / mA cm-2
geo
E vs. RHE / V
b)
ECSA
c)
OER
1.2 1.3 1.4 1.5 1.6
0
20
40
60
80
100
120
j / mA cm
-2
geo
E vs. RHE / V
1.2 1.3 1.4 1.5 1.6
0
20
40
60
80
100
120
j / mA cm
-2
geo
E vs. RHE / V
1.2 1.3 1.4 1.5 1.6
0
20
40
60
80
100
120
j / mA cm
-2
geo
E vs. RHE / V
1.2 1.3 1.4 1.5 1.6
0
20
40
60
80
100
120
j / mA cm
-2
geo
E vs. RHE / V
1.2 1.3 1.4 1.5 1.6
0
20
40
60
80
100
120
j / mA cm
-2
geo
E vs. RHE / V
150 mm/min100 mm/min50 mm/min10 mm/min multilayer
50 nm
120 nm 170 nm
225 nm 480 nm
~ 225 nm ~ 480 nm
~ 170 nm
~ 120 nm
~ 50 nm
a)
SEM
…
…
…
62
(30 mm/min, 4 layers) with intermediate stabilization steps at 200 °C and a final calcination at
375 °C (Figure 25 a, multilayer). ECSA recorded by cyclic voltammetry in the potential
window between 0.40 and 1.40 VRHE shows that the geometrical current response increases
linearly with increasing film thickness (Figure 25 b). Moreover, also the respective OER
scans shift towards lower overpotentials with increasing film thickness (Figure 25 c). The
influence of film thickness on ECSA and OER activity was quantified by analysis of the
respective electrocatalytic data. Figure 26 a plots the obtained total ECSA charge vs. film
thickness, Figure 26 b shows geometric OER current densities at 1.50, 1.53 and 1.55 VRHE
plotted vs. the ECSA for each of the respective single-layer and multi-layer film.
Figure 26: Influence of the thickness of mesoporous templated IrO2 films on ECSA and on OER
performance for single layer (50 – 225 nm) and multilayer catalysts (four layers, 480 nm). a) ECSA as total
charge obtained as a mean value of the integrated anodic and cathodic currents between 0.40 and
1.40 VRHE plotted vs. film thickness (from SEM), b) current density recorded at 1.50 V, 1.53 V and 1.55 VRHE
normalized to the geometric electrode surface area and plotted vs. ECSA. Layer thickness derived from
cross section SEM (Figure 25 a). ECSA and OER cyclic voltammograms are shown in Figure 25 b and
Figure 25 c.
The obtained ECSA scales clearly linear with film thickness for mesoporous IrO2 films
between 50 and 480 nm, indicating that for all films the complete film volume is accessible for
ECSA analysis (Figure 26 a). Moreover, also the geometric current density obtained at a
given potential in OER measurements scales linear with the employed ECSA area (Figure 26
b). This analysis suggests that independent of film thickness each surface site contributes
equally to the OER reaction, even for the thicker films and higher current densities. If any
other process than the surface reaction such as gas transport through the pore system or
electron conduction to the active site was the limiting step a deviation from the linear
behavior would be expected for thicker films at least for the higher potentials and current
densities. Since this is not the case (Figure 26 b) transport limitation are absent in the case of
iridium oxide catalyst films with templated mesopores at least up to 480 nm thickness,
potentials of 1.55 VRHE and current densities as high as 75 mA per cm2 of planar electrode
surface.
0100 200 300 400 500
0
5
10
15
20
ECSA / mC
Layer thickness / nm
single layer multi layer
a) ECSA vs. layer thickness
036912 15 18 21 24
0
10
20
30
40
50
60
70
80
90
100
j at different potentials
vs. RHE / mA cm
-2
ECSA / mC
1.50 V
1.53 V
1.55 V
multi layersingle layer
b) OER activity vs. ECSA
63
In order to relate the achieved catalytic performance to values obtained in previous studies
the overpotentials can be compared at a given geometric current density. Johnson et al.[57]
prepared thick IrO2 layers by dropcasting and obtained OER overpotentials of about
0.240 VRHE at 1 mA/cm². Hu et al.[58] synthesized macroporous IrO2 with colloidal SiO2 via
hard templating and measured ca. 0.250 V overpotential at 1 mA/cm². Nakagawa et al.[141]
used an electro-flocculation method to prepare 2 nm iridium oxide nanoparticles and reported
0.250 V overpotential at 0.5 mA/cm². Reier et al.[63] used spincoating to deposit a lay layer of
Ir-Ni oxide onto titanium and showed an overpotential of 0.258 V at 1 mA/cm². Nong et al.[62]
prepared Ir-Ni oxide nanoparticles with core-shell structure deposited on ATO support.
Subsequently, performed electrocatalytic OER experiments revealed an overpotential of
0.260 V (at 1 mA/cm²). Kushner-Lenhoff et al.[59] synthesized iridium oxide layers via
electrodeposition from Cp*Ir(H2O)3]2+ (Cp* =pentamethylcyclopentadienyl)] and reported
0.267 V at 0.5 mA/cm². A similar synthesis performed by Blakemore et al.[60] led to catalysts
with approximately 0.270 mV overpotential (at 0.5 mA/cm²). Oh et al.[61] successfully
deposited iridium nanodendrites on oxide supports (ATO) and observed an overpotential of
approximately 0.270 V (at 1 mA/cm²). A polycrystalline iridium cylinder measured by Reier et
al.[56] revealed an overpotential of 0.300 V (at 1 mA/cm²). However, investigations of the OER
activity for single crystalline Ir(110) performed by Oezer et al.[137] revealed an overpotential of
0.340 V (at 1 mA/cm²). Ortel et al.[65] achieved 0.220 V (1 mA/cm²) overpotential for thinner
single-layer IrO2. The optimized catalyst of the present study (480 nm thick multilayer
calcined at 375 °C) achieves overpotentials as low as 0.200 V (at 1 mA/cm²), i.e. significantly
lower than previously reported values. A further increase in performance is likely if thicker
films are obtained by further exploitation of the multilayer approach or dip-coating in the
capillary regime.[111]
64
Table 2 Comparison of OER overpotentials at a given current density with previously reported literature
data.
Material
Current density
j / mA cm-2
Overpotential
/ V Reference
Mesoporous templated IrO
2
(multi layer) 1.0 0.200 This work
Mesoporous templated IrO
2
(single layer) 1.0 0.220 Ortel et al.[65]
IrO
2
layer
1.0
0.240
Johnson et al.[57]
Macroporous IrO
2
1.0
0.250
Hu et al.[58]
IrO
2
nanoparticles
0.5
0.250
Nakagawa et al.[141]
Ir-Ni oxide films 1.0 0.258 Reier et al.
[63]
IrNiO
x
nanoparticles on ATO
1.0
0.260
Nong et al.[62]
Electrodeposited IrO2 layer 0.5 0.267 Kushner-Lenhoff et al.
[59]
Ir-Nanodendrites on ATO
1.0
0.270
Oh et al.[61]
Electrodeposited IrO
2
layer
0.5
0.270
Blakemore et al.[60]
Polycrystalline Ir
1.0
0.300
Reier et al.[56]
Single crystalline Ir (110)
1.0
0.340
Oezer et al.[137]
In summary, a new synthesis approach for model-type OER catalysts with controlled
thickness, pore size and crystallinity is reported. In combination with the investigation of
structure-activity relationships the best Ir-oxide based OER catalyst reported so far in
literature is obtained. Mesopores introduced into the catalyst by templating with micelles of
block copolymers enable a rapid transport of the produced oxygen at least up to current
densities of 75 mA/cm2. Thick mesoporous catalyst films are obtained by multilayer
deposition. Even the most active catalyst did not show signs of limitation of electron
transport, electrolyte access or gas transport. The catalyst films are chemically and
mechanically stable also at current densities as high as 115 mA/cm2. The investigation of
structure-activity relationships revealed that the OER performance of mesoporous IrO2 is
controlled by at least two independent factors, i.e. the accessible surface area and the
intrinsic activity per accessible site.
The next chapter will extend the concept to a more complex system, i.e. mixed metal oxides
of iridium and titanium in order to possibly lower the required content of noble metal under
the preservation of OER performance.
65
4.3 Mesoporous templated IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4
Limited availability of Ir, high prices and competition with other applications demand further
improvement of iridium based electrocatalysts in terms of i) activity and ii) stability. In order to
achieve this goal different concepts were reported in literature. i) Hu et al.[142] showed
enhanced iridium mass based OER activities of catalysts consisting of IrO2 deposited on Nb
doped TiO2 nanoparticles prepared by a sol-gel method. ii) Improving the catalytic stability is
considered as another important approach to further increase the sustainability of iridium
based OER catalysts for practical applications such as water splitting. Comninellis et al.[74]
reported that the addition of non conducting oxides such as TiO2, Ta2O5, ZrO2 significantly
decreases the dissolution rate of an active and conductive metal oxide (e.g. IrO2) under
acidic OER conditions. The lower dissolution rate of iridium oxide during OER is explained by
the beginning formation of a solid solution of IrO2 and TiO2. McDaniel et al.[143] reported a
complete formation of a solid solution of IrO2 and TiO2 which was obtained by firing a mixture
of powders from IrO2 and TiO2 at 900 °C and 1000 °C, respectively.
The addition of TiO2 to IrO2 is considered an important approach to improve electrocatalytic
properties of IrO2 which is presented in this thesis. A detailed description of some existing
synthesis routes for mesoporous TiO2 is given in chapter 2.3.2 These pathways comprise
titanium alkoxides and stabilizers,[120] titanium chloride,[105] preformed titanium oxide
nanoparticles,[95] as well as TALH.[109] The synthesis route with titanium alkoxides requires
the use of stabilizing agents. These agents, however, appear less practical during synthesis.
The formation of a solid solution at comparable low temperature is unlikely for synthesis
strategies using preformed TiO2 nanoparticles. Thus, a synthesis route for PEO-PB-PEO
polymer templated IrO2/TiO2 is presented with the use of TiCl4 (chapter 4.3) and TALH
(chapter 4.4), respectively.
Titanium chloride exhibits excellent sol-gel capabilities and is a well investigated precursor
for the production of mesoporous TiO2 via soft templating.[99] Catalytic coatings consisting of
IrO2 and TiO2 were synthesized from Ir(OAc)3 and TiCl4, and physicochemically characterized
(chapter 4.3.1). A controlled variation in calcination temperature was conducted in order to
investigate changes in crystallinity, morphology, electrical conductivity (chapter 4.3.2), as well
as electrochemical activity and surface area (chapter 4.3.3). The varying iridium oxide
loading within titanium oxide is considered as another important synthesis paramater. Thus,
iridium loading was selectively adjusted in order to investigate the influence on morphology,
electrical conductivity (chapter 4.3.4), as well as electrochemical OER activity and surface
area (chapter 4.3.5). The gained knowledge is then combined to identify the OER reaction
controlling parameters that allow the production of highly active OER catalysts.
66
4.3.1 Physicochemical characterization: Ir(OAc)3 and TiCl4 calcined at 400 °C
Films of mesoporous templated IrO2/TiO2 were obtained via dipcoating at 25 °C, 40 %
relative humidity and a withdrawal rate of 150 mm/min on polished substrates (Ti, Si).
Dipcoating solutions were prepared by dissolving Ir(OAc)3, TiCl4 and PEO213-PB184-PEO213 in
ethanol and water. The as prepared samples were dried for 10 minutes in the dipcoating
chamber under controlled atmosphere and subsequently transferred into a preheated muffle
furnace at 400 °C. Physicochemical characterization of the obtained sample is shown in
Figure 27 comprising a, b, c) SEM; d) TEM; e) SAED f, g) SAXS; and h) Kr-physisorption of a
film containing 30 wt. % Ir in Ir/TiO2.
Figure 27: Morphology, composition, crystallinity, pore ordering and surface area of PEO-PB-PEO
templated 30 wt. % Ir in Ir/TiO2 films calcined at 400 °C under air. a) Scanning electron microscopy show
mesoporous templated and untemplated domains at the outer surface plane area. The difference in z-
contrast of both domains is revealed b) for the outer surface plane area in the COMPO image of the
corresponding SEM image as well as for the c) film volume. The emergence of segregrated areas on the
outer surface plane and in the film volume suggest titanium rich mesoporous templated and iridium rich
untemplated domains. Segregation throughout the whole film volume is further confirmed by d) TEM in
high angle annular darkfield mode. e) Selected area electron diffraction measurements show no
pronounced rings suggesting that crystallites are too small to create distinct reflections. Templated
mesoporosity appears to be locally ordered f) parallel (90°, in-plane) and g) perpendicular (20°, out-of-
plane) to the substrate. h) Kr-physisorption reveals 91 m² film surface per m² substrate indicating a fully
accessible pore system.
The SEM images recorded in top view mode (Figure 27 a) reveal two different types of
domains, i.e. an untemplated, textural porous and a mesoporous templated domain
comprising spherical pores with pore openings of 25 ± 4 nm in diameter. The corresponding
100 nm
95 nm
100 nm
a) SEM b) SEM -COMPO d) TEM -HAADF
100 nm
c) cs SEM -COMPO
h) Kr-physisorption
91 m² m
-
²
f) SAXS 90°g) SAXS 20°
0.05 1/nm
0.05 1/nm
1 1/nm
e) SAED
67
FFT of the top view SEM image (inset Figure 27 a) shows an isotropic ring revealing the
presence of an ordered pore arrangement at the outer surface plane area. The periodic
distance between pore centers amounts to approximately 27 nm.
In order to explore the composition of segregated domains, a COMPO image corresponding
to the top view SEM image is shown (Figure 27 b) which indicates the presence of heavier
elements for the untemplated (brighter areas, iridium rich) and lighter elements for the
mesoporous templated (darker areas, titanium rich) domain.
A cross section SEM image in COMPO mode is shown (Figure 27 c) to provide insight into
segregation throughout the whole film volume area. The image reveals a layer thickness of
approximately 95 nm, as well as two domains with different concentration of heavier and
lighter elements. This indicates that segregation of iridium and titanium, which was already
observed in top view SEM (Figure 27 a and b), even occurs within the layer. The observation
is further confirmed by coatings scratched off from the titanium substrate and subsequently
investigated with TEM in high angle annular darkfield mode (Figure 27 d). The image reveals
segregated areas with different brightness, underlining that separation between titanium and
iridium occurs inside the film volume. Furthermore, TEM reveals spherical pores indicating
complete penetration of the coating by templated mesoporosity. A performed electron
diffraction measurement (Figure 27 e) features no pronounced rings which can be attributed
to a crystallite size which is too low for the production of distinct reflections.
The pore ordering was investigated with 2D SAXS data recorded in transmission mode of
layers deposited on titanium foil. The SAXS diffraction patterns of a layer recorded with an
incidient beam angle of 90° (Figure 27 f) and 10° (Figure 27 g) with respect to film surface
normal is shown. The image recorded at 90° (in-plane) displays an isotropic ring suggesting
that domains of PEO-PB-PEO micelles arrange locally ordered parallel to the substrate
(dxy=30 nm). Adjusting an angle of 20° between incident beam and surface normal by tilting
the sample, features an elliptically distorted ring, suggesting locally ordered mesoporosity
perpendicular to the substrate but with slight deformation of the mesopore structure
(dz=8.1 nm). As to the difference in distance of pore centres (d-spacing) parallel (30 nm) and
perpendicular (8.1 nm) to the substrate, the synthesis in its present form produces an
elliptically deformed pore morphology caused by solvent evaporation and film shrinkage
during dip-coating.[101-102, 144]
The surface area of the layer coated on silicon substrate was investigated with krypton as an
adsorbate. The BET surface area amounts to 91 m² film surface area per m² substrate
geometric surface area indicating that most of the containing polymer template was removed
and that an accessible mesopore system is produced. The surface area is in good
agreement with literature reports for thermally prepared mesoporous templated IrO2
synthesized from Ir(OAc)3 and PEO-PB-PEO (130 m²/m²).[65]
68
4.3.2 Influence of calcination temperature on morphology, crystallinity and sheet
conductivity: Ir(OAc)3 and TiCl4 calcined between 200 - 600 °C
Samples of mesoporous templated IrO2/TiO2 were obtained by dipcoating and subsequent
calcination for 10 minutes at temperatures between 80 and 600 °C, respectively. The
obtained samples were analyzed in terms of morphology (SEM, Figure 28 a), crystallinity
(XRD, Figure 28 b, c) and electrical sheet conductivity (Figure 28 d) in order to identify the
impact of calcination temperature.
Figure 28: Influence of calcination temperature on a) morphology, b, c) crystallinity and d) sheet
conductivity of PEO-PB-PEO templated IrO2/TiO2 derived from Ir(OAc)3 and TiCl4 (30 wt. % Ir in Ir/TiO2). a)
SEM micrographs feature segregated areas for samples calcined at different temperatures between 200
and 600 °C, respectively. b) Thermally treated samples at temperatures higher than 500 °C produce
additional reflections that can be assigned to a rutile phase. c) Rietveld refinement was applied for
diffractograms recorded for samples calcined at 600 °C in order to investigate phase composition. d)
Electrical sheet conductivity increases as a function of calcination temperature.
SEM micrographs (Figure 28 a) for films thermally treated at 80 and 200 °C feature
segregated domains and poor contrast. The presence of segregated domains for samples
thermally treated below 200 °C rule out temperature as a driving force for demixing. The
observed poor contrast is related to incomplete polymer template removal.[47] A vast majority
of the polymer template is removed when applying higher calcination temperatures, e.g.
400 °C (Figure 28 a). The electron micrograph reveals two different type of domains, i.e. an
25 30 35 40
100 nm
100 nm
100 nm
600 °C
a) SEM b) XRD
600 °C
400 °C
200 °C
(110) (101)
(101)
(110) (101)
300 °C
500 °C
400 °C
200 °C
200 300 400 500 600
10
-14
10
-12
10
-10
10
-8
10
-6
10
-4
10
-2
10
0
Sheet conductivity / Ohm
-1
sq
T
calc.
/ °C
d) Electrical sheet conductivity
TiO2Rutil
IrO2Rutil
TiO2Anatase
25
2Θ/ °
30 35 40
(101)
(110) (101)
(110) (101)
c) XRD-Rietveld
refinement
600 °C
2Θ/ °
100 nm
80 °C -COMPO
TiO
2
TiCl
4
(400 °C)
IrO
2
Ir(OAc)
3
(375 °C)
Intensity / a.u.
Intensity / a.u.
69
untemplated, textural porous and a mesoporous templated domain. The obtained titanium
rich mesoporous regime shows spherical pores with a pore opening of 25 ± 4 nm in diameter,
whereas the untemplated iridium rich area possesses textural porosity with pore openings
smaller than 2 nm. (also see Figure 27). A further increase of calcination temperature to
600 °C still shows two separated areas. The mesoporous templated titanium rich domain
exhibits smooth pore walls under preservation of mesoporosity, whereas the iridium rich
domain features temperature induced crystal growth leading to loss of textural porosity.
Silicon wafers coated with IrO2/TiO2 and calcined at temperatures between 200 and 600 °C
were investigated by XRD in order to assess the impact of calcination temperature on crystal
properties (Figure 28 b). Samples calcined between 200 and 400 °C do not show distinct
reflections within X-ray diffraction patterns. Hence, the corresponding films appear to be
X-ray amorphous suggesting that the respective oxides of iridium and titanium are either not
crystallized yet or too small to produce diffraction signals. An increase of calcination
temperature to 500 or 600 °C leads to reflections at 2-theta positions of 37.8°, 34.9° and to
an additional shoulder at 36.2°. The reflection pattern at 600 °C was further analyzed by
Rietveld refinement (Figure 28 c). The deconvoluted signals correspond with a IrO2-rutile
phase containing a small fraction of titanium and a TiO2-rutile phase with additional iridium
content. Scherrer equation was applied on the deconvoluted curves in order to reveal the
crystallite size. The obtained values for the respective phases amount to 12 nm (IrO2-rutile
containing Ti) and 6 nm (TiO2-rutile containing Ir).
Figure 28 d presents the influence of calcination temperature for films of IrO2/TiO2 (30 wt. %
Ir in Ir/TiO2) on electrical sheet conductivity. For the purpose of comparison, the sheet
conductivity for similar calcined, mesoporous templated IrO2 and TiO2 coated on glass
substrate is provided by red and green bars (TiO2 synthesized from TiCl4 and calcined for
10 minutes at 400 °C: 2.2·10-13 (Ohm/sq)-1, and IrO2 synthesized from Ir(OAc)3 calcined for
5 minutes at 375 °C: 2.6·10-3 (Ohm/sq)-1). The observed sheet conductivity appears to be low
for samples heat treated at 200 °C and 300 °C, respectively. This observation is in good
agreement with SEM micrographs suggesting incomplete template removal for films calcined
at 200 °C (Figure 28 a) and 300 °C (Figure 44). A further increase of the calcination
temperature steadily increases the electrical sheet conductivity to 2·10-7 (Ohm/sq)-1, probably
related to ongoing crystallite growth and an accompanying decrease in the amount of grain
boundaries.
In summary, three effects are observed: i) a segregation of IrO2 and TiO2 on a lengthscale of
roughly 100 nm, ii) the development of a mesoporous structure solely for titanium rich
domains and iii) a higher degree of textural porosity for iridium rich domains. Based on these
observations, a structural model is deduced and shown in Figure 29. We hypothesize that all
70
three effects can be explained by the different chemical properties of the utilized metal oxide
precursors (e.g. TiCl4 and Ir(OAc)3):
Figure 29: Structural modifications as a function of calcination temperature for 30 wt. % Ir in Ir/TiO2
coatings on titanium synthesized from a solution comprising TiCl4, Ir(OAc)3, PEO-PB-PEO, EtOH and H2O.
Dipcoating was performed under a controlled atmosphere at 25 °C and 40 % relative humidity. The as
prepared samples were dried for 10 minutes in the dipcoating machine and subsequently transferred to a
preheated muffle furnace for calcination at temperatures between 80 and 600 °C, respectively. The
structural models are deduced from observations of physicochemical measurements such as SEM
(Figure 27, Figure 28), TEM (Figure 27), SAXS (Figure 27) and XRD (Figure 28).
Titanium tetrachloride (TiCl4) is a well known precursor often used in syntheses of
nanostructured TiO2 (see chapter 2.2.6 for more detailed information). In literature, it is
reported that TiCl4 shows rather fast hydrolysis and condensation rates.[99, 102] The intrinsic
production of HCl during hydrolysis and condensation prevents further polycondensation.
The result is the formation of self stabilized titanium oligomers terminated by hydroxide
groups with particle diameters in the range between 0.4 - 1.7 nm (reported in literature for
TiCl4 dissolved in EtOH+F127[107]). The presence of accessible hydroxide groups enables the
interaction with hydrolytic regions of the block copolymer (e.g. PEO) through hydrogen
bonding.[99]
iridium acetate is characterized by the presence of acetic acid as a chelat ligand. The
precursor is stable against hydrolysis and condensation in water and ethanol at room
temperature[145] thus forming no small oligomers. The absence of hydroxide groups at the
central atom prevents the interaction of dissolved Ir(OAc)3 and hydrolytic regions of the
polymer template (e.g. PEO).
Based on these reports and the observations from physicochemical analysis within this work,
the above mentioned effects (i-iii) are explained as followed:
i) The equilibrated dipcoating solution comprised small titanium oligomers
(TiCl4-x-y(OEt)x(OH)y, derived by TiCl4), Ir(OAc)3, PEO-PB-PEO, ethanol, and water. The
colloidal suspension appeared clear and showed a light green colour. Tyndall effect usually
occurs for particles dispersed in a liquid medium with a diameter of at least ~100 nm.[146-147]
Thus, it can be concluded that no light is scattered by particles larger than ~100 nm
titanium
Ti rich
rutile
Ir rich
rutile
titanium
Ti rich
phase
titanium
Ir rich
phase
Low crystallinity
Textural
porosity
400 °C 500 °C -600 °C200 °C -300 °C80 °C
titanium
TiCl
4
Ir(OAc)
3
PEO-PB-PEO
Ethanol + H
2
O
Dipcoating
10 min
calcination
Film
deposition
Educts Heat treatment (10 min calcination)
Micelles
71
dispersed in the suspension. The absence of larger particles implies that the observed
segregated domains in catalytic layers are not formed inside the solution. Hence, demixing
very likely occurs after film deposition and is possibly related to different drying behaviours of
iridium and titanium. Different drying behaviours can be associated with different mobilities of
both metal oxide precursors within the dipcoating solution. We hypothesize that the different
mobilities are caused by different interaction behaviours: TiCl4 interacts with the polymer
template, whereas Ir(OAc)3 has no hydroxide groups that may interact with the polymer
template.
Moreover, the different interaction behaviours of TiCl4 and Ir(OAc)3 with the polymer template
are used to describe ii) the development of mesoporosity solely for titanium rich domains. It is
likely to find an oxide precursor next to the polymer template for precursors possessing the
capability to interact with the polymer template (e.g. TiCl4). As a consequence, titanium rich
domains appear to be mesoporous templated, whereas iridium rich domains show no sign of
templated mesoporosity.
However, the iii) iridium rich domains depict a very high degree of textural porosity in contrast
to templated titanium rich domains. This behaviour is associated with the different chemical
structure of the respective precursors. The acetic acid surrounding iridium as a chelat ligand
contains a higher degree of carbon than TiCl4. Carbon containing precursors decompose to
CO2 during calcination which possibly introduces textural porosity to the iridium rich
domains.[65, 148]
4.3.3 OER activity and electrochemical active surface area
Dipcoated films of a solution containing Ir(OAc)3, TiCl4, PEO-PB-PEO, ethanol and water
were calcined in a preheated muffle furnace between 200 and 600 °C. The as received
samples (IrO2/TiO2, 30 wt. % Ir in Ir/TiO2) were subsequently mounted as a working electrode
in a three electrode disc setup using a reversible hydrogen electrode (RHE) as a reference
and a Pt-gauze as a counter electrode. All electrochemical experiments were conducted with
a rotation speed of the working electrode of 1600 rpm, are corrected for iR drop and the
current response is normalized to the substrates geomerical planar surface area. OER
(oxygen evolution reaction) activity was determined by cyclic voltammetry in a potential
window ranging between 1.20 - 1.65 VRHE (6 mV/s, Figure 30 a). Furthermore, the OER
performance is shown as a function of calcination temperature by measuring the
corresponding current density at 1.60 VRHE (Figure 30 b). The ECSA (electrochemical active
surface area) was investigated by cyclic voltammetry in a lower potential window of 0.40 -
1.40 VRHE (50 mV/s, Figure 30 c). The mean value of the integrated anodic and cathodic scan
of each cyclic voltammogram was determined in order to derive a value for the
electrochemical accessible surface area (Figure 30 d).
72
For IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4 (30 wt. % Ir in Ir/TiO2) with different
calcination temperatures Figure 30 shows a) the cyclic voltammograms (CVs) in the OER
regime, b) the quantified OER performance as a function of Tcalc., c) the CVs in the ECSA
region, as well as d) the quantified ECSA in a dependency of Tcalc..
Figure 30: Influence of calcination temperature on a,b) OER performance and c,d) electrochemical
accessible surface area (ECSA) of mesoporous templated IrO2/TiO2 (30 wt. % Ir in Ir/TiO2) on titanium
substrate. a) CVs recorded in the OER potential window between 1.20 and 1.65 VRHE at a scanrate of
6 mV/s, b) current density measured at 1.60 VRHE normalized to the geometric electrode surface area, c)
CVs were recorded in a lower potential window between 0.40 and 1.40 VRHE at 50 mV/s in order to access
electrochemical accessible surface area, d) ECSA is derived as the total charge obtained as a mean value
of the integrated anodic and cathodic currents between 0.40 and 1.40 VRHE. Electrocatalytic data were
accessed in 0.5 M H2SO4 electrolyte with rotating working electrode, RHE reference and Pt gauze counter
electrode. Approximate layer thickness: 100 nm.
Figure 30 a depicts the current response normalized to the titanium sheet’s geometrical
surface area. The current response is directly related to the OER activity and appears to
strongly depend on the applied calcination temperature. Catalysts calcined at 400 and
500 °C show the highest current densities among the studied samples. In order to visualize
the impact of calcination temperature, the OER activity, quantified by measuring the current
density at a potential of 1.60 VRHE, was plotted as a function of calcination temperature
(Figure 30 b). It is clearly visible that the OER activity increases between 200 and 400 °C but
progressively declines with a further increase of calcination temperature.
The ECSA of each sample can be determined from the corresponding current density in the
potential window between 0.40 - 1.40 VRHE as shown in Figure 30 c. The recorded cyclic
voltammograms appear symmetric with respect to the horizontal axis. Samples, heat treated
200 300 400 500 600
0
2
4
6
8
10
12
14
16
j at 1.6 V vs. RHE / mA cm
-2
geo
T
calc.
/ °C
200 300 400 500 600
0
3x10-4
6x10-4
9x10-4
ECSA / C
Tcalc. / °C
1.2 1.3 1.4 1.5 1.6 1.7
0
5
10
15
20
25
30
j / mA cm
-2
geo
E vs. RHE / V
0.4 0.6 0.8 1.0 1.2 1.4 1.6
-0.4
-0.3
-0.2
-0.1
0.0
0.1
0.2
0.3
0.4
j / mA cm
-2
geo
E vs. RHE / V
200 °C
400 °C
600 °C
500 °C
300 °C
200 °C
400 °C
600 °C
500 °C
300 °C
c) active surface area (ECSA)
a) OER performance b) OER performance vs. T
calc.
d) ECSA vs. T
calc.
2nd cycle, iR corrected
73
between 400 and 600 °C, depict a significant current response during the anodic and
cathodic scan. Furthermore, the sample heat treated at 400 °C shows broad humps at
potentials around 0.80 and 0.92 VRHE (marked by arrows). The redox wave at a potential of
~0.92 VRHE is related to the transformation of the IrIII/IrIV redox couple.[125, 136] However, no
clear explanation is found for the presence of the small shoulder at potentials of 0.80 VRHE.
Figure 30 d plots the charge determined by the mean value of the integrated anodic and
cathodic currents in the ECSA range as a function of calcination temperature. The derived
charge is defined as a measure of electrochemical active surface area. Between 200 -
400 °C the ECSA increases with higher calcination temperature, but steadily declines
between 400 and 600 °C for higher calcination temperatures.
The OER activity as well as the electrochemical active surface area show very similar trends.
Electrochemical activity and surface area rapidly increase from 200 to 400 °C and
progressively decrease with further increase of temperature. It is therefore evident that the
accessible surface area contributes to the overall OER activity.
Morphology, crystallinity and electrical sheet conductivity (Figure 28) can now be correlated
to the electrochemical active surface area and OER activity (Figure 30). The low surface area
for samples calcined at 200 and 300 °C (Figure 30 d) is in good agreement with observations
from SEM analysis (Figure 28 a) where poor contrast and brightness was observed. The
appearance of poor contrast and brightness is possibly caused by incomplete polymer
template removal. If the samples still contain remaining polymer residues, the pore system is
still blocked. Thus, no electrochemically accessible surface area (Figure 30 d) as well as no
OER activity (Figure 30 b) is observed. Enhancing the calcination temperature to to 400 °C
forms a mixed metal oxide of iridium and titanium with very low crystallinity (Figure 28 b),
higher electrical sheet conductivity (Figure 28 c) and a high number of accessible active sites
(Figure 30 d). The good accessibilty of the porous structure and the higher electrical sheet
conductivity consequently result in a high OER activity (Figure 30 b). A further increase of the
calcination temperature to 500 and 600 °C forms a well crystallized mixed metal oxide of
iridium and titanium (Figure 28 b) with a loss of textural porosity of the iridium rich domain
(Figure 28 a). Furthermore, the electrical sheet conductivity is increasing, whereas the
observed ECSA progressively decreases at temperatures higher than 500 °C (Figure 30 d).
The strong decline in the ECSA is related to the sintering of the textural porosity induced by
crystal gowth of oxides from iridium and titanium. The activity of polymer templated mixed
oxide films of iridium and titanium is influenced by at least one major factor, i.e. the
accessible surface area.
74
4.3.4 Influence of Ir-content on morphology and sheet conductivity
Mesoporous templated films of IrO2/TiO2 with varying iridium content (0 - 100 wt. % Ir in
Ir/TiO2) were dipcoated on titanium and microscope slides and subsequently calcined for
10 minutes at 400 °C under air. In order to reveal the impact of iridium loading on
morphology and electrical sheet conductivity, the samples were investigated by SEM and
sheet resistivity measurements. The findings of physicochemical characterizations are shown
in Figure 31 for a) SEM and b) electrical sheet conductivity.
Figure 31: Influence of iridium content on the a) morphology and b) electrical sheet conductivity of
mesoporous templated IrO2/TiO2 with different iridium loadings and a subsequent heat treatment at 400 °C
under air. For comparison, the electrical conductivity values of similar prepared, mesoporous templated
IrO2 (Ir(OAc)3, 5 min 375 °C) and TiO2 (TiCl4, 10 min 400 °C) are added as green and red lines, respectively.
SEM images recorded in top view mode (Figure 31 a) for samples with 15 wt. % Ir in Ir/TiO2
and heat treated at 400 °C reveal two different type of domains, i.e. untemplated, textural
porous and mesoporous templated domains with spherical pores. The elemental composition
of both domains was investigated by COMPO (Figure 27 b) revealing the presence of heavier
elements for the untemplated (brighter areas, iridium rich) and lighter elements for the
mesoporous templated (darker areas, titanium rich) domains. The segregation between both
metal oxides (Ir, Ti) is still present with increasing iridium content up to loadings of 75 wt. % Ir
in TiO2. Segregation of both metal oxides is explained by the distinct chemical properties of
the utilized precursor systems, i.e. Ir(OAc)3 and TiCl4 (see chapter 4.3.2 for detailed
explanation of demixing). However, the distance between iridium rich areas decreases as the
iridium loading within TiO2 increases.
a)SEM
b) Electrical sheet conductivity
100 nm 100 nm 100 nm 100 nm 100 nm
15wt.%Ir/TiO
2
30wt.%Ir/TiO
2
45wt.%Ir/TiO
2
60wt.%Ir/TiO
2
75wt.%Ir/TiO
2
020 40 60 80 100
10-14
10-12
10-10
10-8
10-6
10-4
10-2
100
Sheet conductivity / Ohm-1 sq
wt. % Ir in Ir/TiO2
TiO
2
TiCl
4
(400 °C)
IrO
2
Ir(OAc)
3
(375 °C)
75
The electrical sheet conductivity was determined for different loadings of IrO2 within TiO2
coated on insulating glass and subsequently heat treated at 400 °C under air. For the
purpose of comparison, the sheet conductivity for similar calcined, mesoporous templated
IrO2 and TiO2 coated on glass substrate is provided by red and green bars (TiO2 synthesized
from TiCl4 and calcined for 10 minutes at 400 °C: 2.2·10-13 (Ohm/sq)-1 and (IrO2 synthesized
from Ir(OAc)3 calcined for 5 minutes at 375 °C: 2.6·10-3 (Ohm/sq)-1). The iridium content has
a severe impact on electrical sheet conductivity (Figure 31 b). It increases with higher iridium
content which is related to the metallically conductive character of IrO2.[54]
4.3.5 Influence of Ir-content on electrochemical OER activity and surface area
The effect of iridium content on morphology and sheet conductivity can now be correlated
with OER activity and electrochemical accessible surface area. Films of mesoporous
templated IrO2/TiO2 with different loadings of iridium were obtained via dipcoating on polished
titanium sheet substrates. The OER activity was determined by cyclic voltammetry in a
potential window ranging between 1.20 - 1.65 VRHE (6 mV/s, 1600 rpm iR corrected, Figure
32 a). Furthermore, the OER performance at a potential of 1.60 VRHE is shown as a function
of iridium loading within TiO2 (Figure 32 b). The ECSA (electrochemical active surface area)
was investigated by cyclic voltammetry in a lower potential window between 0.40 - 1.40 VRHE
(50 mV/s, Figure 32 c). The mean value of the integrated anodic and cathodic scan of each
cyclic voltammogram was determined in order to derive a value for the electrochemical
accessible surface area. The ECSA is shown in dependency of iridium loading (Figure 32 d).
For IrO2/TiO2, derived from Ir(OAc)3 and TiCl4 (400 °C) with different iridium loadings in TiO2,
Figure 32 depicts a) the cyclic voltammograms in the OER regime, b) the quantified OER
performance as a function of iridium content, c) CVs in the ECSA region, as well as d) the
quantified ECSA as a function of iridium loading.
76
Figure 32: Influence of iridium content on a,b) OER performance and c,d) electrochemical accessible
surface area. a) CVs recorded in the OER regime between 1.20 - 1.65 VRHE (6 mV/s), b) current density
recorded at 1.60 VRHE with respect to geometrical surface area, c) cyclic voltammograms recorded in the
ECSA range between 0.40 - 1.40 VRHE (50 mV/s), d) ECSA derived as the total charge obtained as a mean
value of integrated anodic and cathodic currents.
The OER performance of each catalyst (IrO2/TiO2, 400 °C) with different iridium loading was
accessed by cyclic voltammetry. Figure 32 a shows the current response normalized with
respect to the titanium sheet’s geometrical surface area. All catalysts except for the sample
with a loading of 15 wt. % Ir in Ir/TiO2 depict a significant OER activity. However, increasing
the loading to 30 wt. % Ir leads to a higher OER performance. The OER activity was
quantified by measuring the current density at potentials of 1.60 VRHE. In order to visualize
the influence of the iridium loading on the electrocatalytic performance, Figure 32 b shows
the quantified OER activity as a function of iridium loading. The OER activity steadily
increases with higher iridium content.
The corresponding ECSA of each sample was investigated by cycling the potential between
0.40 - 1.40 VRHE (50 mV/s) as depicted in Figure 32 c. The varying iridium content shows a
severe impact on the current response. The recorded cyclic voltammograms feature a
symmetric behaviour with respect to the horizontal axis. All samples show broad redox-
waves at potentials of ca. 0.94 VRHE indicating the presence of a IrIII/IrIV redox couple.[125, 136] In
order to quantify the impact of iridium loading on the active surface area, Figure 32 d shows
the charge determined by the mean value of the integrated anodic and cathodic currents in
the ECSA range as a function of iridium loading. The determined charge is understood as a
measure of electrochemical active surface area. The ECSA steadily increases with higher
010 20 30 40 50 60 70 80 90100
0
10
20
30
40
50
60
70
80
j at 1.6 V vs. RHE / mA cm
-2
geo
wt. % Ir in Ir/TiO2
1.2 1.3 1.4 1.5 1.6 1.7
0
10
20
30
40
50
60
70
80
j / mA cm
-2
geo
E vs. RHE / V
010 20 30 40 50 60 70 80 90100
0
1x10-3
2x10-3
3x10-3
4x10-3
ECSA / C
wt. % Ir in Ir/TiO
2
0.4 0.6 0.8 1.0 1.2 1.4 1.6
-2.0
-1.5
-1.0
-0.5
0.0
0.5
1.0
1.5
2.0
j / mA cm-2
geo
E vs. RHE / V
15 wt%
30 wt%
60 wt%
75 wt%
15
30
60
75
c) Active surface area (ECSA)
a) OER performance b) OER performance
vs. Ir-content
d) ECSA vs. T
calc.
100
wt.%Ir
100 wt%
2nd cycle, iR corrected
77
iridium content. It is clear to see that the OER activity and ECSA follow similar trends as they
steadily increase with increasing iridium content. Thus, it is obvious that ECSA has a severe
influence on the overall OER activity.
Morphology and electrical sheet conductivity (Figure 31) of IrO2/TiO2 calcined at an
intermediate temperature (400 °C, low crystallinity, Figure 28) can now be correlated to the
OER activity and ECSA. Samples with a loading of 15 wt. % Ir in Ir/TiO2 exhibit a very low
ECSA (Figure 32 d). The morphology is characterized by the presence of a mesoporous
system (Figure 31 a). Furthermore, charging was absent as SEM images were recorded
indicating that most of the polymer template was removed during heat treatment. The active
surface area of a catalytic coating is expected to scale linear with the amount of active
centres, e.g. iridium loading within TiO2. An increase of the iridium loading from 15 wt. %
(6.8 mol %) to 30 wt. % (15.1 mol %) Ir in Ir/TiO2 enhances the amount of active centres by
ca. 2.2. However, the electrochemical active surface area is enhanced by ca. 20 times
(Figure 32 d). The discrepancy to the expected behaviour suggests that other effects than
the amount of active centres influence the active surface area. Stoerzinger et al.[78] observed
an enlarged distance of redox peaks for LaCoO3 on different electrical conductive substrates.
For low conductivity these redox peaks have the greatest distance to the equilibrium
potential. Hence, samples with a low electrical conductivity suffer from a larger voltage drop
over the layer. As a consequence, these samples suffer from a decreased electrocatalytic
reactivity. In the case of IrO2/TiO2, the observed sheet conductivity, however, does not scale
linearly with the amount of iridium (Figure 31 b). It is therefore required to further explore the
exact impact of conductivity on the electron transport and the resulting effects on intrinsic
reactivity. A more detailed discussion can be found in the chapters 4.4.4 - 4.4.6 for IrO2/TiO2
synthesized from Ir(OAc)3 and TALH.
If electrons travelling through the catalytic layer are hindered by an insufficient degree of
electrical conductivity the presence of two different reactivity regimes are expected, i.e. i) a
high surface area with a high OER activity for samples with a sufficient degree of electrical
conductivity and ii) a low surface area with a low OER activity for samples showing an
insufficient electrical conductivity.
78
4.4 Mesoporous templated IrO2/TiO2 synthesized from Ir(OAc)3 and TALH
Catalytic films of mesoporous templated IrO2/TiO2 derived by Ir(OAc)3 and TiCl4 show large
segregated areas with diameters larger than approximately 100 nm. The process of demixing
is associated with the different chemical behaviours of both metal oxide precursors in
solution (see chapter 4.3.2). In order to obtain well mixed metal oxides of titanium and
iridium, two possible pathways are imaginable.
The first route includes an IrO2 precursor with the capability to undergo hydrolysis and
condensation processes. As a consequence this may lead to the interaction with the polymer
template and hydrolyzed titanium species. In the second pathway a TiO2 precursor is
incapable to interact with the polymer template, thus being chemical more similar to Ir(OAc)3.
However, dipcoated films, obtained by solutions prepared with IrCl3·xH2O instead of Ir(OAc)3
and TiCl4, exhibit small iridium rich domains even at low loadings (15 wt. % Ir in TiO2) and
low calcination temperatures (325 °C, Figure A3). The present demixing between both metal
oxides suggest that the usage of IrCl3·xH2O and TiCl4 is not suitable for the preparation of
well mixed metal oxides of iridium and titanium.
Therefore, the second pathway must be taken into consideration. Titanium(IV)
bis(ammonium lactato)dihydroxide (TALH) is well known to act as a suitable metal oxide
precursor for the successful synthesis of mesoporous templated TiO2 (see chapter 2.3.2).[109]
TALH is characterized by a titanium cation (oxidation state +IV) complexed by lactic acid
which functions as a chelat ligand, and two hydroxide groups. It was reported that TALH
does not undergo hydrolysis and condensation when dissolved in water.[149] Iridium acetate
shows a similar behaviour as it is complexed by acetic acid, thus stabilised against hydrolysis
and condensation when dissolved in water and ethanol at room temperature.[145] The
similarity of both metal oxide precursors is considered as an important factor for the
synthesis of mixed metal oxides.
Chapter 4.4.1 illustrates the structure of IrO2/TiO2 dipcoated from a solution containing
Ir(OAc)3, TALH metal oxide precursors and PEO-PB-PEO polymer template and heat treated
for 10 minutes at 400 °C. The influence of calcination temperature on morphology,
crystallinity and electrical conductivity is investigated (4.4.2). Furthermore, the obtained
information are then correlated with electrocatalytic OER activity and active surface area in
order to deduce structure-activity relations (4.4.3). The amount of active iridium within TiO2 is
considered as another important synthesis parameter. Chapter 4.4.4 studies the impact of
iridium loading on morphology and electrical conductivity. The electron transport processes
within the catalytic layer (4.4.5) are investigated in detail and correlated with the
electrocatalytic OER activity and intrinsic reactivity (4.4.6). The combined knowledge is used
to elucidate the impact of electrical conductivity on the intrinsic reactivity.
79
4.4.1 Physicochemical characterization (Ir(OAc)3 and TALH)
Catalytic coatings of mesoporous IrO2/TiO2 on polished silicon and titanium susbtrates were
obtained by dipcoating a solution of PEO213-PB184-PEO213 polymer template, Ir(OAc)3, TALH,
methanol and water. Dipcoating was performed at a withdrawal rate of 150 mm/min, an
ambient temperature of 25 °C and a relative humidity of 40 %. Thereafter, the as prepared
samples remained in the dipcoating chamber for 10 minutes to assure evaporation of volatile
residues, such as ethanol. Subsequently, the samples were transferred into a preheated
muffle furnace and calcined at 400 °C under air. The obtained samples contain a nominal
iridium content of 30 wt. % Ir in Ir/TiO2. Figure 33 shows the physicochemical
characterization data obtained by a, b) SEM; c, d) TEM; e) SAED; f) integrated SAED; g, h)
SAXS and i) Kr-physisorption.
Figure 33: Morphology, composition, pore ordering and surface area for samples dipcoated on silicon and
titanium from a solution of PEO-PB-PEO, Ir(OAc)3, TALH, methanol and water (30 wt. % Ir in Ir/TiO2).
Subsequently, heat treatment was conducted under air at 400 °C. a) SEM micrographs feature a fully
developed pore system at the outer surface plane area as well as a homogenous distribution of IrO2 and
TiO2. The film volume area was investigated by b) cross section SEM in COMPO mode, TEM at c) lower
magnification and d) higher magnification. The obtained e) SAED diffraction pattern features broad
isotropic rings indicating that the mesopore walls consist of nanocrystallites. f) The corresponding
integrated SAED image was used to assign crystalline phases (see text for detailed explanation). SAXS
measurements feature g) isotropic (90°) and h) ellipsoidal shaped (20°) rings suggesting the presence of
locally ordered mesopores parallel and perpendicular to the substrate. i) Kr-physisorption provides a
surface area of 136 m² film surface per m² substrate indicating a fully accessible pore system.
In order to assess the pore morphology and the distribution of iridium oxide in titanium oxide,
a top view SEM image was recorded and is presented in Figure 33 a. The coating exhibits
a) SEM d) HR -TEMb) cs SEM -COMPO
i) Kr-physisorption
g) SAXS 90°h) SAXS 20°
100 nm 2 nm
136 m² m
-2
80 nm
e) SAED
anatase
rutile
c) TEM
20 nm
1 1/nm
0.05 1/nm
0.05 1/nm
5.0 4.0 3.0 2.0 1.0
Intensity / a.u.
d-spacing / Å
* TiO2Anatase
# TiO2Rutile
○IrO2Rutile
*
*
○
***
#
○
#
○
#
#
#
○
○
PDF(00-021-1276)
PDF(00-015-0870)
PDF(00-021-1272)
f) SAED -integrated
80
spherical pores on the outer surface plane area with a diameter of 29 ± 6 nm. These pores
are slightly larger than for PEO-PB-PEO templated IrO2 synthesized from Ir(OAc)3
(16 nm[65]), and for PEO-PB-PEO templated TiO2 derived by TiCl4 (21 nm[98]). The larger pore
diameter is most likely induced by swelling of the polymer template due the high water
content in the purchased TALH precursor solution (contains 50 wt. % H2O). The FFT image
(inset of Figure 33 a) of the corresponding SEM image features an isotropic ring, suggesting
an ordered pore arrangement with a periodic distance of approximately 32 nm between pore
centers. The film volume was investigated by cross section SEM in COMPO mode for
samples coated on silicon substrate and is shown in Figure 33 b. The obtained micrograph
depicts a layer thickness of 80 nm.
The mesoporous templated IrO2/TiO2 were further investigated by TEM in order to provide
more detailed data regarding morphology (Figure 33 c, d) and crystallinity (Figure 33 e). The
TEM micrograph at low magnification (Figure 33 c) shows spherical pores suggesting a
complete penetration of the coating by templated mesoporosity. High resolution TEM image
(Figure 33 d) features small dark spherical areas attributed to a higher content of iridium
indicating segregation on a length scale of 1 - 2 nm. Furthermore, distinct lattice fringes are
revealed suggesting the presence of nanocrystallites within the pore walls. In order to assess
information about the crystal phases, selected area electron diffraction (SAED)
measurements were performed. Figure 33 e depicts SAED data for films containing 30 wt. %
Ir in TiO2 as well as the reference data for IrO2 rutile (PDF: 00-015-0870) and TiO2 anatase
(PDF: 00-021-1272). The resolution of the SAED measurement is too low to clearly
distinguish between crystal phases of IrO2 rutile and TiO2 rutile. However, the obtained SAED
pattern features isotropic rings leading to the conclusion that the pore wall is composed of
randomly oriented nanocrystallites assigned to TiO2 anatase as well as IrO2 rutile and/or TiO2
rutile (Figure 33 f), as well as an unknown amount of crystallites too small in size to produce
distinct diffraction signals. Due to the broad appearance of the diffraction rings, caused by a
very low crystallite size and by similar lattice parameters for IrO2 rutile and TiO2 rutile, the
presence of either IrO2 rutile, TiO2 rutile or a mixture of both can not be distinguished.
The local pore arrangement of layers deposited on titanium foil was investigated with 2D-
SAXS data recorded in transmission mode. SAXS pattern of IrO2/TiO2 films recorded with an
incident beam angle of 90° (Figure 33 g) feature an isotropic ring indicating locally ordered
mesoporosity parallel to the substrate. The scattering images for tilted samples at angles of
20° (Figure 33 h) show ellipsoidal shaped rings suggesting locally ordered mesoporosity
perpendicular to the substrate. The film exhibits d-spacings of 40 nm (in-plane, 90°) and
10 nm (out of plane, 20°) representing an elliptically deformed pore morphology.
Kr-physisorption was used in order to assess the surface area of IrO2/TiO2 layers derived
from Ir(OAc)3 and TALH coated on silicon substrate. The BET surface area amounts to
81
136 m² film surface area per m² substrate geometric surface area (layer thickness: 80 nm).
An almost fully removed polymer template as well as an accessible porous system
(Figure 33 i) is formed. The surface area for mesoporous templated films synthesized from
Ir(OAc)3 and TiCl4 amounts to 91 m²/m² (layer thickness: 95 nm). The significant higher
surface area for TALH based films is most likely caused by the higher degree of textural
porosity within the pore walls. The latter is probably induced by the formation of CO2 from the
decomposition of TALH and Ir(OAc)3 during thermal treatment.[65]
4.4.2 Influence of calcination temperature on morphology, crystallinity and electrical
conductivity
Calcination temperature can have a severe impact on morphology, crystallinity and electrical
conductivity. Mesoporous templated films of IrO2/TiO2 were dipcoated from a solution
containing Ir(OAc)3 and TALH (30 wt. % Ir in Ir/TiO2) and calcined at temperatures between
200 and 600 °C, respectively. The obtained films were characterized in terms of morphology,
crystallinity and electrical sheet conductivity. For the differently heat treated samples Figure
34 shows the corresponding a) SEM micrographs, b) X-ray diffraction patterns, c) Rietveld
refinement and d) electrical sheet conductivity.
Figure 34: Impact of thermal treatment on a) morphology, b, c) crystallinity and d) electrical sheet
conductivity for PEO-PB-PEO templated IrO2/TiO2 (30 wt. % Ir in Ir/TiO2) synthesized from Ir(OAc)3 and
TALH. a) Samples calcined at 200 °C exhibit charging suggesting incomplete polymer template removal.
An increase of the calcination temperature to 400 °C reveals a fully developed pore system, whereas
100 nm
100 nm
100 nm
25 30 35 40
600 °C
400 °C
200 °C
a) SEM b) XRD
600 °C
400 °C
200 °C
TiO
2
Rutile
IrO
2
Rutile
(110) (101)
TiO
2
Anatase(101)
(110) (101)
200 300 400 500 600
10-14
10-12
10-10
10-8
10-6
10-4
10-2
100
Sheet conductivity / Ohm
-1
sq
T
calc.
/ °C
d) Electrical sheet conductivity
2Θ/ °
25 30 35 40
(101)
(110) (101)
(110) (101)
c) XRD-Rietveld
refinement
TiO
2
TALH
(400 °C)
IrO
2
Ir(OAc)
3
(375 °C)
Intensity / a.u.
Intensity / a.u.
2Θ/ °
82
higher calcination (600 °C) induces crystal growth. b) The larger crystallite size for calcination at 600 °C is
confirmed by XRD due to the additional reflections which appear in the corresponding diffractogram. c)
Rietveld refinement was applied for diffractograms recorded for samples at 600 °C in order to investigate
the phase composition. d) Sheet conductivity is shown for samples calcined at temperatures between 200
- 600 °C and for comparison, of IrO2 synthesized from IrOAc (375 °C) and TiO2 obtained by TALH (400 °C).
SEM micrographs for samples calcined at 200 °C (Figure 34 a) show a grainy texture and a
bright horizontal line throughout the whole image. The grainy appearance of the image and
the observed higher partial brightness may signify incomplete removal of the polymer
template. Furthermore, no large segregated domains in the range of > 5 nm are observed
suggesting a thorough mixture of IrO2 and TiO2. An increase in calcination temperature to
400 °C (Figure 34 a) feature a fine granulated SEM micrograph with good contrast and
brightness. The presence of a fine grained SEM image is possibly related to the removal of
most of the polymer template. Furthermore, the mesopore walls are characterized by textural
porosity. However, calcination at 600 °C (Figure 34 a) causes a distortion of spherical
mesopore shape and leads to a decreasing textural porosity associated with the onset of
sintering. The SEM image further depicts small particles arising on the outer surface plane
area. These particles are possibly related to temperature induced crystallite growth of an
iridium rich oxide.
The corresponding films were further characterized by XRD (Figure 34 b) in order to relate
the morphological changes to the crystal properties. Mesoporous layers heat treated
between 200 and 400 °C do not provide reflection signals that can clearly be associated with
crystalline phases. The derived samples are therefore either amorphous or possess
crystallites too small in diameter for sufficient production of intense reflection signals. An
increase in calcination temperature to 600 °C provides XRD patterns with reflections at 2-
theta positions of 25.3°, 27.9°, 34.8° and a small shoulder at 35.0°. Rietveld refinement was
conducted for further analysis of the crystal phases. The deconvoluted curves of the
corresponding XRD pattern for samples calcined at 600 °C (Figure 34 c) are assigned to TiO2
anatase, TiO2-rutile (containing Ir) and IrO2-rutile (containing Ti) indicating the formation of
solid solutions. The respective crystallite sizes obtained by the Scherrer-equation amount to
5 nm (TiO2-anatase), 12 nm (TiO2-rutile containing Ir) and 21 nm (IrO2-rutile containing Ti).
The electrical sheet conductivity was analyzed as a function of calcination temperature and is
shown in Figure 34 d. For the purpose of comparison, the sheet conductivity of similar
calcined, mesoporous templated IrO2 and TiO2 coated on glass substrate is provided by red
and green bars, respectively (TiO2 synthesized from TALH (400 °C): 7.1·10-10 (Ohm/sq)-1,
IrO2 synthesized from Ir(OAc)3 (375 °C): 2.6·10-3 (Ohm/sq)-1). Samples calcined at 200 °C
exhibit low sheet conductivity. This observation is in good agreement with SEM images that
implied incomplete template removal. The electrical sheet conductivity strongly increases for
samples thermally treated at temperatures between 300 and 400 °C. This behavior is
83
explained by the removal of most of the polymer template and the formation of
nanocrystallites. The formation of nanocrystallites strongly decreases the amount of grain
boundaries which is associated with a faster electron transport. However, a further increase
of calcination temperature reduces sheet conductivity. We hypothesize, that the decrease in
sheet conductivity at high calcination temperatures (600 °C) is possibly attributed to the
aggregation of IrO2 which in turn is caused by crystallite growth. As a consequence of
enhanced crystallite growth, the preliminary connected and conductive IrO2 network is
interrupted. Thus, the electron transport through the catalytic layer is decelerated.
The obtained data from the physicochemical characterisation of Figure 33 and Figure 34 was
used to derive a structural model which is shown in Figure 35. The model describes
temperature induced changes in morphology and crystallinity of IrO2/TiO2 synthesized from a
dipcoating solution containing TALH, Ir(OAc)3, PEO-PB-PEO, methanol and water. In Figure
35 the samples show i) a thorough mixture of IrO2/TiO2 up to intermediate calcination
temperatures (400 °C), ii) a textural porosity throughout the mesopore walls, iii-1) a
temperature induced demixing and iii-2) the beginning formation of a solid solution for
samples heat treated above ca. 500 °C.
Figure 35: Structural changes as a function of calcination temperature for 30 wt. % Ir in Ir/TiO2 coatings on
titanium prepared from a solution containing TALH, Ir(OAc)3, PEO-PB-PEO, MeOH and H2O. Dipcoating
was performed under a controlled atmosphere at 25 °C and 40 % relative humidity. The as prepared
samples were dried for 10 minutes in the dipcoating chamber and subsequently transferred to a
preheated muffle furnace for calcination at temperatures between 80 and 600 °C, respectively. The
structural models are deduced from observations of physicochemical measurements such as SEM
(Figure 33, Figure 34), TEM (Figure 33), SAXS (Figure 33) and XRD (Figure 34).
i) The utilized metal oxide precursors, i.e. Ir(OAc)3 and TALH are characterized by sterically
demanding chelat ligands, such as acetic acid and lactic acid, respectively. Reports from
literature claim that both metal oxide precursors appear stable to hydrolysis and
condensation when dissolved in water.[145, 149] The absence of hydrolysis and condensation
prevents the formation of hydroxide groups which in turn prevents the interaction with
400 °C 500 °C -600 °C200 °C -300 °C80 °C
TALH
Ir(OAc)
3
PEO-PB-PEO
Methanol + H
2
O
Dipcoating
10 min
calcination
Film
deposition
Educts Heat treatment (10 min calcination)
TiO
2
anatase
Ir rich
phase
Ti rich
phase
titaniumtitanium
TiO
2
anatase
titaniumtitanium
Textural
porosity Ir rich
rutile
Ti rich
rutile
Low crystallinity,
mixed rutile ?
84
hydrolytic regions of the polymer template. Thus, Ir(OAc)3 and TALH exhibit similar chemical
reactivity in solution.
Film deposition on titanium substrate followed by a heat treatment at 200 °C reveals a
thorough mixture of IrO2 and TiO2 (Figure 34 a), possibly due to a similar drying behavior of
Ir(OAc)3 and TALH. This behavior is associated with equal interaction properties with the
polymer template. Both metal oxide precursors tend to show no attractive interaction with the
polymer template as they lack of hydrolysis and condensation. Therefore, we hypothesize
that a higher chemical similarity between the used metal oxide precursors such as Ir(OAc)3
and TALH causes a more homogenously distributed mixed metal oxide, e.g. IrO2 and TiO2.
ii) An increase in calcination temperature to 400 °C features a fully developed pore system
(Figure 34 a) with textural porosity in the mesopore walls. The textural porosity is possibly
introduced by the combustion of carbon to CO2 from both metal oxide precursors.[65]
However, TEM studies (Figure 33 d) reveal small (ca. 2 nm), segregated areas which appear
darker in brightfield mode suggesting an iridium rich domain. SAED images (Figure 33 e) of
the corresponding samples show diffraction rings which can be assigned to a mixture of TiO2-
anatase and rutile. The broadness of the diffraction rings and the similar lattice parameters of
TiO2-rutile and IrO2-rutile neither allow a clear distinction of both rutile phases (IrO2 and TiO2)
nor a mixture thereof. The derived scheme (Figure 35) therefore shows TiO2 anatase, small
iridium rich phases, and titanium rich phases, from which the latter two possibly crystallized
in a mixed rutile structure.
iii) Due to a further increase in calcination temperature, a distortion of the spherical mesopore
shape can be observed. The arising crystallites appear iridium rich. XRD measurements
(Figure 34 b) show distinct reflection signals which can be assigned to TiO2 anatase, TiO2
rutile containing Ir (Ti-rich rutile), and IrO2 rutile containing Ti (Ir-rich rutile). Obviously, two
effects occur when calcination temperatures higher than 500 °C are applied: iii-1) thermally
induced demixing, and iii-2) the beginning formation of a solid solution. Tammann[150]
reported that atoms can change places within crystallites or at the interface between two
different crystallite species, if a sufficient degree of atom oscillation (temperature dependent)
is reached. In honour of Tammann, this particular temperature is called the Tammann
temperature. He further found[150] that metals must be heated to ca. 1/3 of their melting
temperature in order to form a solid solution. In case of oxides from titanium and iridium, the
Tammann temperature TTammann has the followed values:
TiO2: TTammann = 791 °C[151]
IrO2: TTammann = 413 °C[152]
iii-1) The lower Tammann temperature of IrO2 in comparison to TiO2 allows mobility at much
lower temperatures than required for TiO2. Thus, thermally induced demixing of IrO2/TiO2
should start for samples calcined at temperatures above ca. 400 °C. In fact, samples heat
85
treated at 400 °C show only a very low degree of demixing between IrO2 and TiO2 (Figure
33). Samples heat treated at 500 °C, however, clearly depict larger areas with iridium rich
crystallites. iii-2) A further increase in calcination temperature to 600 °C forms a demixed
solid solution of IrO2 and TiO2. We assume, that an incorporation of TiO2 by surrounding IrO2
crystallites is initiated which results in fractions of iridium rich rutile and titanium rich rutile. In
literature, the formation of a phase pure solid solution between IrO2 and TiO2 [143] was
achieved by exceeding the Tammann temperature with a mixture of IrO2-powder and TiO2-
powder (900 °C). However, simply enhancing the calcination temperature in the presented
mesoporous templating synthesis approach would lead to excessive crystallite growth and, in
consequence to a complete loss of textural porosity as well as mesoporosity. Furthermore,
the underlying titanium substrate might oxidize to form a rather thick insulating layer of TiO2.
Thick layers of TiO2 are known to cause an additional voltage drop over the layer, further
inhibiting electrocatalytic reactivity.[153]
4.4.3 Influence of calcination temperature on electrochemical OER activity and surface
Mesoporous templated films of IrO2/TiO2 (30 wt. % Ir in Ir/TiO2) were prepared on titanium
sheet substrates by dipcoating and subsequent calcination for 10 minutes under air at
temperatures between 200 - 600 °C, respectively. The obtained samples were mounted as a
working electrode within a RDE setup. A reversible hydrogen electrode served as the
reference and a platinum gauze as the counter electrode. All electrochemical experiments
were conducted at a speed of rotation of 1600 rpm in 0.5 M H2SO4. During electrochemical
investigations, the resulting current response was normalized to the substrate’s geometrical
planar surface area and the potential was corrected for iR drop. The OER (oxygen evolution
reaction) activity was determined by cyclic voltammetry in a potential window ranging
between 1.20 - 1.65 VRHE (6 mV/s, Figure 36 a). Furthermore, the OER performance is
shown as a function of calcination temperature by measuring the corresponding current
density at 1.60 VRHE (Figure 36 b). The ECSA (Electrochemical active surface area) was
investigated by cyclic voltammetry in a lower potential window of 0.40 - 1.40 VRHE (50 mV/s,
Figure 36 c). The mean value of the integrated anodic and cathodic scan of each cyclic
voltammogram was determined in order to derive a value for the electrochemical accessible
surface area. The ECSA is shown in dependency of the calcination temperature (Figure 36
d).
For IrO2/TiO2 synthesized from Ir(OAc)3 and TALH (30 wt. % Ir in Ir/TiO2) with different
calcination temperatures Figure 36 shows a) cyclic voltammograms recorded in the OER
regime, b) the quantified OER performance as a function of calcination temperature, c) cyclic
voltammograms in the ECSA region, and d) the calcination temperature dependent quantified
ECSA.
86
Figure 36: Impact of calcination temperature on a, b) OER performance and c, d) electrochemical
accessible surface area (ECSA) for 30 wt. % Ir in Ir/TiO2 synthesized from Ir(OAc)3 and TALH. a) CVs
recorded in the OER potential window between 1.20 and 1.65 VRHE at a scanrate of 6 mV/s, b) current
density measured at 1.60 VRHE normalized to the geometric electrode surface area, c) CVs recorded in a
lower potential window between 0.40 and 1.40 VRHE at 50 mV/s are used to access the electrochemical
accessible surface area, d) ECSA is derived as the total charge obtained as a mean value of the integrated
anodic and cathodic currents between 0.40 and 1.40 VRHE. Electrocatalytic data were recorded in
0.5 M H2SO4 with a rotating working electrode, a RHE reference and a Pt gauze counter electrode.
The OER activity for samples of IrO2/TiO2 synthesized from Ir(OAc)3 and TALH is shown in
Figure 36 a. The observed current density is defined as a measure of OER activity and
appears to be strongly dependent on the applied calcination temperature. However, only
catalysts calcined at 400 °C show a significant OER activity. The corresponding cyclic
voltammogram features a typical exponential relationship as stated by the Butler-Volmer
equation. The impact of calcination temperature on the OER activity was quantified by
measuring the OER activity at potentials of 1.60 VRHE. Figure 36 b shows the OER activity as
a function of calcination temperature. It is clearly visible that the OER activity increases within
a temperature window of 200 - 400 °C, whereas a further increase to 500 and 600 °C
strongly decreases the OER activity.
The corresponding electrochemical active surface area (ECSA) of each sample was
accessed by measuring the current density in a lower potential window of 0.40 - 1.40 VRHE
(Figure 36 c). The obtained “ECSA-CVs” are symmetrical with respect to the horizontal axis.
The observed current density in the anodic and cathodic scan appear to be affected by the
1.2 1.3 1.4 1.5 1.6 1.7
0
5
10
15
20
25
30
j / mA cm-2
geo
E vs. RHE / V
0.4 0.6 0.8 1.0 1.2 1.4 1.6
-0.4
-0.3
-0.2
-0.1
0.0
0.1
0.2
0.3
0.4
j / mA cm
-2
geo
E vs. RHE / V
200 °C
400 °C
600 °C
500 °C
300 °C
200 °C
400 °C
600 °C
500 °C
300 °C
c) active surface area (ECSA)
a) OER performance b) OER performance vs. Tcalc.
d) ECSA vs. Tcalc.
200 300 400 500 600
0
3x10
-4
6x10
-4
9x10
-4
ECSA / C
T
calc.
/ °C
200 300 400 500 600
0
2
4
6
8
j at 1.6 V vs. RHE / mA cm
-2
geo
T
calc.
/ °C
2nd cycle, iR corrected
87
applied calcination temperature. Samples calcined at 400 °C depict by far the largest current
response, thus the highest ECSA. Furthermore, all CVs feature redox waves at a potential of
ca. 0.92 VRHE which are associated with the equilibrium potential of the IrIII/IrIV redox
couple.[125, 136] In order to further analyze the relationship between ECSA and OER activity,
the total charge, obtained as a mean value of the integrated anodic and cathodic scans of
CVs from the ECSA regime, is plotted as a function of calcination temperature (Figure 36 d).
The derived charge is used as a measure for ECSA. Samples heat treated at 200 and 300 °C
do not exhibit a significant ECSA. However, the ECSA shows the highest values at
calcination temperatures of 400 °C but strongly decreases with further increasing the
calcination temperature.
The OER activity as well as the electrochemical active surface area show very similar trends
as a function of calcination temperature. Samples heat treated at intermediate temperatures
(400 °C) show a high ECSA as well as a high electrochemical OER activity. Therefore, we
conclude that the electrochemical accessible surface area is considered as an important
oxygen evolution reaction controlling parameter and contributes to the overall OER activity.
The influence of morphology, crystallinity and sheet conductivity can now be related to the
oxygen evolution reaction (OER) activity as well as to the electrochemical accessible surface
area (ECSA) in order to deduce structure-activity relationships. Samples heat treated at 200
and 300 °C exhibit no significant ECSA (Figure 36 d) which is in line with SEM (Figure 34 a).
Here, a grainy texture and partially charging was observed which indicates that the sample
has an insufficient degree of electrical conductivity which in fact was observed with sheet
resistivity measurement (Figure 34 c). If the sample still comprises remaining polymer
template residues, it appears likely that the pore system is not accessible, thus neither ECSA
(Figure 36 d) nor OER activity (Figure 36 b) is observed. An increase in calcination
temperature to 400 °C forms a material with increased electrical conductivity (Figure 34 c),
low crystallinity (Figure 34 b), and a throughout mixture of iridium oxide and titanium oxide
(Figure 34 a). Furthermore, a strong increase is observed for the ECSA (Figure 36 d) and the
OER activity (Figure 36 b). The tremendous increase in the ECSA is related to the removal of
most of the polymer template which creates an accessible pore system, thus a higher overall
OER activity. At calcination temperatures of 500 and 600 °C an induced crystallite growth
(Figure 34 b) accompanied by the formation of not phase pure i) titanium rich rutile, ii) iridium
rich rutile, and iii) anatase (Figure 35) is observed. Moreover, a decrease occurs in textural
porosity (Figure 34 a) and electrical conductivity (Figure 34 c). Also, the ECSA strongly
(Figure 36 d) decreases. The tremendous degradation of the ECSA is related to the loss of
textural porosity by the onset of sintering which in turn is caused by the temperature induced
crystallite growth of oxides from iridium and titanium. Due to the very similar trends of OER
88
activity and ECSA as a function of calcination temperature the assumption can be made that
the activity of polymer templated mixed oxide films of iridium and titanium is influenced by at
least one major factor, i.e. the accessible surface area.
4.4.4 Influence of Ir-content on morphology and sheet conductivity
Mesoporous templated layers of IrO2/TiO2 with different iridium loadings (0 - 100 wt. % Ir in
Ir/TiO2) were deposited on silicon and glass substrates by dipcoating and subsequent
calcination for 10 minutes at 400 °C under air. The effects of iridium concentration on
morphology and electrical conductivity of the catalytic IrO2/TiO2 films were analyzed by SEM
and resistivity measurements. For samples with different iridium content Figure 37 shows a)
SEM micrographs and b) electrical sheet conductivity of corresponding samples dipcoated on
glass substrates.
Figure 37: Impact of iridium content on a) morphology (on silicon) and b) sheet conductivity (on glass) for
mesoporous templated IrO2/TiO2 systems synthesized from Ir(OAc)3 and TALH and subsequently heat
treated at 400 °C under air. a) SEM micrographs depict a homogenous dispersion of IrO2 and TiO2 b)
Sheet conductivity remains constant for iridium loadings of 25 wt. % Ir in Ir/TiO2. A further increase of the
iridium content significantly enhances sheet conductivity.
Figure 37 a illustrates the morphology at the outer surface plane area for films of IrO2/TiO2
with a different amount of iridium. The SEM micrographs feature a homogenous mixture of
IrO2 and TiO2 without large (ca. 100 nm) aggregated domains regardless of the iridium
content. All samples exhibit spherical pore openings. However, pore openings increase in
size with higher titanium content from 23.1 nm (75 wt. % Ir) to 30.3 nm (15 wt. % Ir). The
effect of the water containing TALH-solution (50 wt. % H2O) is a higher ratio of water to
020 40 60 80 100
10-14
10-12
10-10
10-8
10-6
10-4
10-2
100
Sheet conductivity / Ohm
-1
sq
wt. % Ir in Ir/TiO
2
a) SEM
10 nm 10 nm 10 nm 10 nm 10 nm
15wt. %Ir/TiO230wt. %Ir/TiO245wt. %Ir/TiO260wt. %Ir/TiO275wt. %Ir/TiO2
b) Electrical sheet conductivity
TiO
2
TALH
(400 °C)
IrO
2
Ir(OAc)
3
(375 °C)
89
polymer template within the dipcoating solution. This leads to a swelling of formed micelles,
thus larger pore openings.
In Figure 37 b the influence of the iridium content on the electrical sheet conductivity is
featured. For the purpose of comparison, the sheet conductivity of similar calcined,
mesoporous templated IrO2 and TiO2 coated on glass substrate, is provided by green and red
bars, respectively (TiO2 (TALH, 10 min 400 °C): 7.1·10-10 (Ohm/sq)-1, IrO2 (Ir(OAc)3 5 min 375
°C: 2.6·10-3 (Ohm/sq)-1). The electrical conductivity remains unaffected up to an iridium
content of 20 wt. % Ir in TiO2 and stays constant within a range of 0.7·10-9 to
4·10-9 (Ohm/sq)-1. However, an increase of the iridium loading to 25 wt. % in TiO2 enhances
the electrical conductivity to 4.5·10-9 (Ohm/sq)-1. At iridium contents higher than 30 wt. % in
TiO2 a significant improvement of the electrical sheet conductivity with higher iridium content
is observed. Pure, mesoporous templated IrO2 shows the highest electrical sheet conductivity
which equals to 2.6·10-3 (Ohm/sq)-1. Normalizing this value for a layer thickness of 50 nm
results in a specific conductivity of 5.1·104 S/m (5.1·102 S/cm) which is considered as
metallically conductive[54] and is in good agreement with values reported in literature ranging
from 4.3·105 S/m[154] to 2·106 S/m.[155]
The observed electrical sheet conductivity for IrO2/TiO2 coatings, synthesized from Ir(OAc)3
and TALH on glass substrates, strongly depend on the added amount of iridium. The
insignificant changes in the electrical conductivity for mesoporous templated TiO2, with
loadings ranging between 5 - 25 wt. % Ir in Ir/TiO2, is potentially related to the incomplete
connection of conductive IrO2 chains. The insulating TiO2 positioned between conductive
domains of IrO2 hinders fast electron transport through the layer. The electrical sheet
conductivity significantly increases for samples with iridium loadings higher than 30 wt. % Ir
in Ir/TiO2. The addition of a sufficient amount of iridium oxide might connect conductive IrO2
chains. The electrical conductivity is therefore enhanced as electrons must not longer travel
through insulating TiO2 domains. A further increase in iridium loading progressively increases
the electrical sheet conductivity as there is a further amount of metallically conducting IrO2
present. The observed behaviour is in good agreement with the percolation theory which
describes the electrical conductivity of conductive materials (e.g. IrO2) within an insulating
matrix (e.g. TiO2).[74, 77]
90
4.4.5 Influence of Ir-content on electron transport resistance and electrochemical
active surface area
Electrochemical investigations for IrO2/TiO2 layers with different content of iridium on titanium
substrates were conducted in order to determine the impact of iridium loading on the electron
transport resistance through the film, on the electrochemical active surface area (ECSA) and
also on the oxygen evolution reaction (OER) performance. The IrO2/TiO2 layer was coated on
titanium substrate and employed as a working electrode in a rotating-disc electrode (RDE)
setup. A Pt-mesh and a RHE were used as a counter and reference electrode, respectively.
0.5 M H2SO4 served as an electrolyte solution. ECSA[125] measurements were performed at a
lower potential regime between 0.40 -1.40 VRHE and a sweeprate of 50 mV/s. The applied
potential was iR-corrected and the resulting current response was normalized to the
electrode’s planar geometric surface area. Every figure shows the 2nd cycle.
For mesoporous templated IrO2/TiO2 (Ir(OAc)3+TALH) layers with different iridium loadings
deposited on titanium sheets Figure 38 shows the a, b) cyclic voltammograms recorded in
the ECSA regime (0.40 - 1.40 VRHE). As a function of iridium loading, Figure 38 shows c) the
redox peak position from the “ECSA-CVs” and the d) quantified ECSA.
Figure 38: Influence of iridium loading on a, b) CVs recorded in the ECSA potential window between 0.40 -
1.40 VRHE at a sweep rate of 50 mV/s, c) the redox peak positions E0 for the (IrIII/IrIV) couple obtained by the
corresponding CVs recorded in the ECSA regime and d) the quantified ECSA. a, b) Enhanced current
density and a drift in peak positions is observed as a function of iridium content. c) The redox peak
potentials are plotted depending on the iridium content. A clear spreading of the redox peaks away from
the equilibrium potential E0(IrIII/IrIV) is observed for samples with iridium loadings lower than 20 wt. % Ir in
020 40 60 80 100
0.0
0.2
0.4
0.6
0.8
1.0
1.2
E vs. RHE / V
wt. % Ir in Ir/TiO
2
a) ECSA
(5 -100 wt % Ir)
c) Redox peak positions d) ECSA vs wt. % Ir
0.4 0.6 0.8 1.0 1.2 1.4
-1.2
-0.8
-0.4
0.0
0.4
0.8
1.2
j / mA cm
-2
geo
E vs. RHE / V
5
20
100 wt. % Ir
75
60
45
30
020 40 60 80 100
0
2x10
-3
4x10
-3
ECSA / C
wt. % Ir in Ir/TiO
2
15
E
0
b) ECSA
(5 -30 wt % Ir)
0.4 0.6 0.8 1.0 1.2 1.4
-0.3
-0.2
-0.1
0.0
0.1
0.2
0.3
j / mA cm
-2
geo
E vs. RHE / V
5
20
30 wt. % Ir
15
10
91
Ir/TiO2. This observation is associated with an insufficient degree of electrical conductivity. d) The mean
value of the integrated anodic and cathodic charge of the recorded CVs shows a successive increase of
ECSA as a function of iridium loading. All samples were coated on titanium substrates followed by
thermally treatment at 400 °C under air.
Figure 38 a and b show the current response of IrO2/TiO2 layers on titanium substrates
recorded in a lower potential window of 0.40 - 1.40 VRHE. The current response is normalized
to the electrode’s geometrical surface area and is composed of contributions from the double
layer capacitance and faradayic currents. Currents related to the double layer capacitance
are recorded over the whole potential window, whereas faradayic currents show pronounced
broad peaks at a specific equilibrium potential which is associated with a Ir+III/Ir+IV redox
couple. Our thermally prepared mesoporous layers of IrO2/TiO2 coated on titanium substrates
show a peak potential at 0.92 VRHE which is in good agreement with values found in literature
(0.90 VRHE[64] and 0.95 VRHE[125]) for similar prepared IrO2. Faradayic currents of highly
hydrated IrO2 are the result when reacting in terms of a proton-inclusion-mechanism which is
described as followed[156]:
IrOx(OH)y + δ H+ + δ e- IrOx-δ(OH)y+δ
Considering this equation, a decrease in the iridium content leads to a reduced number of
iridium centres, and hence a drop in the current density as noticeable in Figure 38 a.
However, when lowering the iridium content, the peaks are still pronounced (Figure 38 b).
Similar prepared mesoporous templated “iridium free” TiO2 coatings on titanium substrate
show no significant contribution to the current density. Therefore, we assume that for mixed
IrO2/TiO2 systems with different loadings of iridium, the appearing peaks are caused by
faradayic currents related to the Ir+III/Ir+IV redox couple. However, a clear shift of the peak
position to higher (anodic scan) and lower (cathodic scan) potentials is visible for iridium
loadings lower than 20 wt. % Ir in Ir/TiO2 (Figure 38 c).
The quantification of peak positions as a function of iridium content in TiO2 is shown in Figure
38 c. The redox peaks at approximately 0.92 ± 0.01 VRHE of pure mesoporous templated IrO2
(100 wt. % Ir) are ascribed to the equilibrium voltage of the Ir+III/Ir+IV redox couple.[64, 125]
Redox peaks are still located near the equilibrium voltage with an iridium content as low as
20 wt. % Ir in Ir/TiO2. A further decrease of the iridium loading significantly spreads the redox
peaks away from the equilibrium voltage (Figure 38 c). In the latter case, the electron
transport is hindered through layers of IrO2/TiO2.
The electron transport through bulk materials, such as unporous LaCoO3, has been
investigated by Stoerzinger et al.[78]. LaCoO3 was deposited on three substrates with different
conductivity by pulsed laser epitaxy. To investigate, the influence of the electron transport
through the layer as a function of conductivity, the peak positions of the [Fe(CN)6]3-/4- redox
92
couple were analyzed. They observed an enlarged distance of the redox peaks from the
equilibrium potential for samples with lower conductivity. Thus, the higher resistivity of these
samples induces a voltage drop over the layer.
Samples with iridium loadings of at least 20 wt. % Ir in Ir/TiO2 exhibit redox peaks positioned
near the equilibrium potential, suggesting a sufficient degree of electrical conductivity.
Additional ex-situ measurements for electrical resistivity (Figure 37 b) showed a significant
increase of conductivity for samples with a slightly higher iridium loading of at least 30 wt. %
Ir in Ir/TiO2. Therefore, we hypothesize that the samples need to be at least conductive as
approximately 3·10-8 (Ohm/sq)-1 (ca. 0.1 S/m) in order to provide a sufficient electron
transport through the layer and perform as highly active OER catalysts.
In Figure 38 d the electrochemical accessible surface area (ECSA) is plotted as a function of
iridium loading. The ECSA corresponds to the transferred charge in the cyclic
voltammograms (CVs) of Figure 38 a and was obtained by the mean value of the integrated
cathodic and anodic scan for each CV. The differing iridium content within TiO2 has a severe
impact on the ECSA. This observation is in good agreement with the expected proton-
inclusion-mechanism of IrO2. The faradayic current response within the ECSA-CVs is
associated with the transformation of the Ir+III/Ir+IV redox couple. It is therefore plausible, that
an increasing iridium amount within TiO2, normalized with respect to the planar geometrical
surface area, leads to a higher ECSA.
4.4.6 Influence of Ir-content on OER performance and intrinsic activity
Mesoporous templated IrO2/TiO2 with different iridium loadings were dipcoated on titanium
sheet substrates from a solution of Ir(OAc)3 and TALH. The as prepared samples were dried
in the dipcoating chamber under controlled atmosphere and subsequently transferred into a
preheated muffle furnace. All samples were calcined at 400 °C under air atmosphere. The
obtained samples were employed as the working electrode within a rotating-disc electrode
setup. The OER performance was investigated in a potential window of 1.20 - 1.65 VRHE with
a scan rate of 6 mV/s. The applied potential was iR-corrected and the resulting current
response was normalized with respect to the electrode’s planar geometric surface area.
For different loadings of iridium within TiO2 Figure 39 shows a) the 2nd iR-corrected cyclic
voltammograms in the OER regime, b) the quantified OER activity at potentials of 1.60 VRHE;
c, d) the quantified charge as a measure of electrochemical active surface area (ECSA).
93
Figure 39: Impact of iridium content in IrO2/TiO2, synthesized from Ir(OAc)3 + TALH, dipcoated on titanium
sheets and subsequently heat treated at 400 °C on a) CVs recorded in the OER regime, b) OER activity at
1.60 VRHE and c, d) relationship between OER activity and ECSA. a) CVs recorded in the OER regime in a
potential window between 1.20 - 1.65 VRHE. b) The OER activity increases as a function of iridium content.
c) The Intrinsic activity is derived by a linear fit between OER activity and ECSA. d) The difference in OER
activity and linear fit for samples with lower iridium content suggest a decrease in intrinsic activity.
The OER activity in Figure 39 a is measured for samples with iridium contents between
15 wt. % - 100 wt. % Ir (pure IrO2). The current response was normalized to the substrate’s
planar geometric surface area (0.1965 cm²). Samples with iridium loadings higher than
20 wt. % Ir in Ir/TiO2 are more active in the OER than samples with lower loadings of iridium.
The OER performance increases for higher iridium loadings. In order to visualize the
increase in the OER performance, the current density at 1.60 VRHE was measured and is
plotted as a function of the iridium content (Figure 39 b).
Figure 39 b shows the current density values at 1.60 VRHE of equally prepared and measured
samples with loadings between 0 - 100 wt. % Ir in Ir/TiO2. A low current density is observed
for samples with loadings below 20 wt. % Ir in Ir/TiO2. However, at iridium loadings of
25 wt. % Ir in Ir/TiO2 and higher, the observed OER activity successively increases.
In Figure 39 c the quantified OER activity of all samples is plotted as a function of ECSA. The
OER activity of iridium loadings between 30 - 100 wt. % Ir in Ir/TiO2 is linearly dependent on
the ECSA (fixed intercept at 0). The OER performance is increased by 16.4 mA/cm² for every
1·10-3 ECSA [C] (R²=0.998).
In Figure 39 d, only the current response for samples with loadings between 0 and
25 wt. % Ir is displayed. The dashed line is the extrapolated linear fit from the 30 -
0.0 2.0x10-3 4.0x10-3
0
10
20
30
40
50
60
70
80
j at 1.60 V vs. RHE / mA cm
-2
geo
ECSA / C
1.2 1.3 1.4 1.5 1.6 1.7
0
10
20
30
40
50
60
70
80
j / mA cm
-2
geo
E vs. RHE / V
15
30
60
75
100wt%Ir
(IrO
2
)
2nd cycle, iR corrected
a) OER performance b) OER performance regimes
020 40 60 80 100
0
10
20
30
40
50
60
70
80
j at 1.60 V vs. RHE / mA cm
-2
geo
wt. % Ir in Ir/TiO
2
100 wt%Ir
75
60
45
30
25
20
IrO
2
0.0 2.0x10
-4
4.0x10
-4
0
1
2
3
4
j at 1.60 V vs. RHE / mA cm-2
geo
ECSA / C
10
0-5
15
20
25 wt.% Ir
d) OER activity vs. ECSA
(0 -25 wt % Ir)
c) OER activity vs. ECSA
(0 -100 wt % Ir)
20x10
-4
40x 10
-4
94
100 wt. % Ir region (Figure 39 c). The current densities at a potential of 1.60 VRHE are
significantly lower than expected by the extrapolated linear fit from the 30 - 100 wt. % Ir
region. This discrepancy between the observed and the expected current density suggest a
different intrinsic electrocatalytic reactivity of IrO2 dispersed within TiO2.
Two different regimes are observed within the OER-ECSA plot (Figure 39 c and d) for
IrO2/TiO2 synthesized from Ir(OAc)3 and TALH: i) a linear relation for samples with loadings
higher than ca. 30 wt. % Ir in Ir/TiO2, and ii) a discrepancy from the expected linear behaviour
for samples with loadings lower than ca. 30 wt. % Ir in Ir/TiO2. In order to explain both
regimes, a correlation with the electrocatalytic and physicochemical properties of the
corresponding samples is provided.
i) Samples with iridium loadings higher than 20 wt. % Ir feature redox peaks associated with
the Ir+III/Ir+IV redox couple located close to the thermodynamic equilibrium (Figure 38 c).
Samples with loadings higher than 30 wt. % Ir show a significant increase in the electrical
sheet conductivity (Figure 37 b) as a function of iridium loading. Both observations suggest a
sufficient degree of the electrical conductivity. Thus, no additional voltage drop over the layer
is expected that potentially might diminish electrocatalytical processes. In chapter 4.2.5 a
linear dependency between the OER activity and ECSA up to current densities of ca.
80 mA/cm² was observed for mesoporous IrO2 (Figure 26 b). Prior conducted investigations
on the electrical conductivity (Figure 37 b, Figure 38 c) and the OER-ECSA scaling relation
(Figure 26 b) are in good agreement with the linear dependency between the OER activity
and the ECSA for IrO2/TiO2 samples with loadings higher than 30 wt. % Ir in TiO2
(Figure 39 c). The combined data thus suggest that IrO2 dispersed in TiO2 has the same
intrinsic electrocatalytic reactivity as mesoporous templated IrO2.
ii) Samples with loadings lower than 20 wt. % Ir in Ir/TiO2 show peak potentials in the ECSA
regime spreading away from the equilibrium voltage of the Ir+III/Ir+IV redox couple
(Figure 38 c). For samples with loadings less than or equal to 30 wt. % Ir the observed
electrical sheet conductivity attains a value too small to provide a sufficient electron transport
through the layer (Figure 37 b). The consequence is an additional voltage drop over the layer
which in turn lowers the electrocatalytic reactivity. The higher overpotential appears as a
discrepancy from the expected linear relationship between the OER and the ECSA
(Figure 39 d). Therefore it is evident, that an iridium loading of at least 30 wt. % Ir in TiO2
and/or a sheet conductivity higher than approximately 3·10-8 (Ohm/sq)-1 (ca. 0.1 S/m) must
be provided in order to ensure a sufficient electron transport through the layer and to further
avoid additional voltage drops.
In conclusion, active iridium centres in mixed IrO2/TiO2 systems exhibit the same intrinsic
activity as in pure IrO2, if a sufficient degree of conductivity is provided.
95
4.5 Reference catalysts
A detailled electrocatalytic investigation of commercial reference catalysts appears to be
mandataroy in order to incorporate our new mesoporous systems into a more global context.
Commercial available powders consisting of IrOx/TiOx and IrO2 were considered as relevant
systems for the sake of comparison. The powders were separately dispersed in iPrOH, milliQ
H2O and Nafion, (see 3.1.6 and 3.1.7 for detailed procedure) and subsequently ultrasonified
for 15 minutes in order to obtain “inks”. A defined volume from each of the inks was pipetted
onto titanium cylinders, followed by a drying step at 60 °C. The obtained samples were
analyzed physicochemically (SEM) and electrochemically (OER).
Chapter 4.5.1 shows SEM images of IrOx/TiOx and IrO2 on titanium cylinders at different
magnifications to identify the morphology of the dropcasted powders. The OER activity is
discussed in chapter 4.5.2 and was derived in an acidic electrolyte solution. In addition, the
iridium mass base related OER activity is determined in order to identify the commercial
system with higher activity. Finally, chapter 4.5.3 shows the geometrical OER activity for the
higher active system (e.g. IrOx/TiOx) as a function of iridium loading to investigate the
reproducibility of the synthesis approach and to identify signs of transport limitations.
4.5.1 SEM
In order to investigate the morphology of commercial available catalysts, dispersions of
IrOx/TiOx or IrO2 were dropcasted onto titanium cylinders (A = 0.1963 cm²). The prepared
samples were dried at 60 °C and finally investigated by SEM. Recorded electron micrographs
are shown in Figure 40 for a) IrOx/TiOx (“Elyst”) and b) IrO2.
Figure 40: Morphology of different commercial available catalysts deposited by an “ink procedure” on
titanium substrates. The used inks consisted of iPrOH, H2O, Nafion and a) IrOx/TiOx (“Elyst”) or b) IrO2.
a) IrO
x
/TiO
x
(Elyst 750480,
Umicore)
b) IrO
2
(Sigma Aldrich)
10 kx 20 kx 50 kx 200 kx
1000 nm 1000 nm 100 nm100 nm
1000 nm 1000 nm 100 nm100 nm
96
Figure 40 a depicts electron micrographs recorded for IrOx/TiOx “Elyst”. It is clearly visible
that particles with different sizes are present. A rough estimation of the particle size reveals a
distribution between ca. 50 - 1000 nm. Furthermore, the particles appear to be randomly
distributed onto the substrate’s surface without any sign of ordering. An enhanced
magnification shows that the surface of grains is characterized by stripes with brighter and
darker appearance. It appears that a homogenous particle size distribution cannot be
achieved by ultrasonification. The inhomogenous distribution of grains on the substrate might
be a result of the drying behavior during dropcasting. The difference in contrast and
brightness on the particle surface suggest textural roughening.
Scanning electron microscopy images shown in the bottom row feature the morphology of
IrO2 (Figure 40 b). A particle size distribution similar as for IrOx/TiOx is observed. It is visible
that particles with a size roughly between 50 and 1000 nm are present. However, these
particles appear to be randomly distributed on the surface indicating that the synthesis in its
present form does not lead to the production of homogenous catalytic coatings. Images
recorded with higher magnifications depict large areas of IrO2 grains on the surface with
comparable contrast and brightness. The smooth particle interface is often associated with a
crystalline character.
Both commercial available catalysts feature a broad particle size distribution and appear to
be inhomogenously distributed on the titanium substrate. However, powders of IrOx/TiOx
(Figure 40 a) tend to show a higher degree of textural roughening, whereas IrO2 (Figure 40 b)
depicts a smooth outer surface area.
4.5.2 OER activity
Dropcasted layers of IrOx/TiOx and IrO2 on titanium cylinders served as the working electrode
in a rotating disc electrode setup. The OER activity was determined by cycling the potential
between 1.20 – 1.65 VRHE at 6 mV/s. Current responses were normalized with respect to the
substrate’s planar geometrical surface area and were corrected for iR drop. Figure 41 shows
for commercial systems (IrOx/TiOx and IrO2) the a) 2nd and 25th CV and the b) iridium mass
based OER activity at potentials of 1.55 VRHE during the anodic scan of the corresponding
CVs
97
Figure 41: a) Geometrical and b) iridium mass based OER activity for commercial systems comprising
IrOx/TiOx and IrO2. Commercial catalysts were dropcasted by an ink procedure onto titanium cylinders and
subsequently investigated electrochemically. The resulting OER activity of the commercial catalysts is
shown within the a) 2nd and 25th CV. By measuing the current at 1.55 VRHE during the anodic scan of the
corresponding CVs, the b) nominal iridium mass based OER activity (unit: A/gIr) was derived. (1.20 -
1.65 VRHE, 6 mV/s, 1600 rpm, 0.5 M H2SO4, nominal iridium mass)
For IrOx/TiOx and IrO2 coated on titanium cylinders Figure 41 a shows the 2nd and 25th iR
corrected cyclic voltammograms. Both catalysts show a decrease in the OER related current
density after 25 consecutive cycles. The observed current density of IrOx/TiOx (“Elyst”) is
higher than for IrO2 during the 2nd and 25th cyclic voltammogram. However, the nominal
iridium loading on the substrate must be considered, which is 1.55 times higher for the
IrOx/TiOx catalyst than that of IrO2. In order to identify the commercial system with the higher
mass base related iridium activity and to quantify the decrease in current density, the current
was measured at 1.55 VRHE during the anodic scan of the corresponding CVs and normalized
with respect to the nominal iridium loading. Figure 41 b depicts the iridium mass based OER
activity of IrOx/TiOx and IrO2. IrOx/TiOx shows a decrease of 31 % in current density from 4.5
(2nd CV) to 3.1 (25th CV) A/gIr. The iridium mass based current of IrO2, however, reduces it’s
activity by 25 % from 2.8 (2nd CV) to 2.1 (25th CV) A/gIr. A similar decrease in the mass
related OER activity suggests that both catalysts are equally stable. However, IrOx/TiOx
shows a 1.6 times higher mass base related OER activity than IrO2, and thus is identified as
the more active commercial catalyst.
1.2 1.3 1.4 1.5 1.6 1.7
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
j / mA cm
-2
geo
E vs. RHE / V
1.2 1.3 1.4 1.5 1.6 1.7
0.0
0.2
0.4
0.6
0.8
1.0
1.2
1.4
1.6
1.8
2.0
j / mA cm
-2
geo
E vs. RHE / V
0
2
4
6
8
10
Iridium mass based OER activity
at 1.55 V vs. RHE / A g
-1
Ir
0
2
4
6
8
10
Iridium mass based OER activity
at 1.55 V vs. RHE / A g
-1
Ir
25
th
iR corrected CV
IrO
x
/TiO
x
„Elyst“
20.3 µg
Ir
cm
-2
IrO
2
13.1 µg
Ir
cm
-2
IrO
x
/TiO
x
„Elyst“
20.3 µg
Ir
cm
-2
IrO
2
13.1 µg
Ir
cm
-2
2
nd
iR corrected CV
IrO
2
13.1 µg
Ir
cm
-2
IrO
x
/TiO
x
Elyst
20.3 µg
Ir
cm
-2
IrO
2
13.1 µg
Ir
cm
-2
IrO
x
/TiO
x
Elyst
20.3 µg
Ir
cm
-2
a) OER activity
b) Iridium mass
based OER
activity
98
4.5.3 Influence of catalyst loading onto titanium substrate on OER activity
Chapter 4.5.2 revealed a higher mass base related OER activity for commercial catalysts of
IrOx/TiOx (“Elyst”) than IrO2. To further investigate the reproducibility of the dropcasting
synthesis approach and to identify any limitations, different loadings of IrOx/TiOx on titanium
cylinders were produced. The amount of ink volume that can be pipetted on a titanium
cylinder at once is limited by the size of the droplet which must not overflow along the
borders of the substrate. Therefore, we multi-dropcasted only small volumes of an “IrOx-TiOx
ink” accompanied by intermediate drying steps at 60 °C in order to vary the iridium loading
within a wide range. The achieved loading range of iridium onto titanium cylinders (A =
0.1963 cm²) was about 4 - 800 µgIr (ca. 20 - 4075 µgIr/cm²).
The impact of the nominal iridium loading on the current density at 1.56 VRHE during the
anodic scan is shown for the a) 2nd CV and b) 25th CV (Figure 42).
Figure 42: Influence of the nominal iridium mass of catalytic systems of IrOx/TiOx (“Elyst”) on the
geometrical current density in the OER regime. The current density at 1.56 VRHE during the anodic scan is
shown for the a) 2nd and b) 25th CV. Cyclic voltammograms were obtained by sweeping the potential
between 1.20 - 1.65 VRHE at 6 mV/s (1600 rpm, 0.5 M H2SO4, Pt-mesh).
Figure 42 a depicts the geometrical current response at 1.56 VRHE during the anodic scan of
the 2nd CV as a function of the nominal iridium mass. A clear linear relationship between the
current density and the nominal iridium loading up to current densities as high as ca.
80 mA/cm² (1.56 VRHE) and nominal iridium loadings of ca. 800 µgIr can be observed with a
slope of 0.103 mA/cm² per 1 µgIr (R²=0.994). The plot in Figure 42 b is equally derived for the
25th CV. The lower slope of 0.051 mA/cm² per 1 µgIr (R²=0.978) indicates that these catalysts
exhibit a lowered mass related performance. However, the clear presence of a linear
relationship between the OER activity and the iridium mass at 2 and 25 consecutive CVs
indicates the absence of transport limitation and reveals a good reproducibility of the
synthesis approach. The obtained OER overpotential at 1 mA/cm² for a sample with a
nominal iridium loading during the 2nd CV amounts to 0.248 V, which is in good agreement
with values reported in literature, e.g. 220 mV.[65]
0200 400 600 800 1000
0
10
20
30
40
50
60
70
80
90
100
j at 1.56V vs. RHE / mA cm
-2
geo
Nominal iridium mass / µg
IrOx/TiOx
„Elyst“
0200 400 600 800 1000
0
10
20
30
40
50
60
70
80
90
100
j at 1.56 V vs. RHE / mA cm
-2
geo
Nominal iridium mass / µg
IrOx/TiOx
„Elyst“
b) 25th iR corrected CVa) 2nd iR corrected CV
99
5 General discussion
The obtained knowledge from the chapters 4.2 and 4.5 are now used to establish a general
discussion (chapter 5) in order to identify trends valid for all catalytic coatings operating
under acidic conditions, i.e. IrO2 and IrO2/TiO2. Synthesis parameters such as calcination
temperature, crystallinity, electrical conductivity, electrochemical active surface area (ECSA)
and layer thickness were identified as the most relevant OER-controlling parameters.
Furthermore, the applied overpotential during electrocatalytic investigation showed to
possess an impact on kinetical aspects, i.e. Tafel slope.
The general discussion shows the structure and morphology of TiO2, IrO2 and IrO2/TiO2 as a
function of the applied precursors (e.g. TiCl4, TALH, Ir(OAc)3), mixtures thereof (chapter 5.1),
and as a function of calcination temperature (5.2). The observed morphology is then used to
develop a scheme (5.3) in which most of the relevant structural aspects of all systems are
shown. In order to identify OER-controlling parameters, convenient plots are presented to
demonstrate the influence of calcination temperature (5.4), crystallinity (5.5), electrical
conductivity (5.6), and layer thickness (5.7) on OER activity. Moreover, Tafel slopes were
determined and discussed for i) mesoporous templated IrO2 as a function of layer thickness
(5.7); and ii) IrO2 and IrO2/TiO2 as a function of calcination temperature (5.8) and iridium
loading (5.9). The data are then combined to deduce structure-activity relations (5.10). For
the most relevant systems, according to the structure-activity relations, a comparison of the
iridium mass based OER activity between the reference catalysts and the new catalysts from
this work will be established (5.11).
100
Figure 43: Different precursor systems were used to derive different categories of mesoporous templated oxides, such as TiO2 (1st and 2nd row), IrO2 (3rd row) and
IrO2/TiO2 (4th and 5th row). The precursors: TiCl4, TALH and Ir(OAc)3 have different chemical natures, thus highly affecting the appearance of mesopores as well as pore
walls (SEM: top view and high resolution, see text for detail description). All samples show similar layer thicknesses (SEM: cross section) and templated mesoporosity
within the film volume area (TEM). Crystallinity was investigated by SAED showing TiO2-anatase (1st and 2nd row),[98, 109] IrO2-rutile (3rd row), low crystalline/amorphous
IrO2/TiO2 (4th row), and a mixture of TiO2 anatase and rutiles of TiO2 and IrO2 (propably forming a solid solution) (5th row).
95 nm
100 nm
p)
100 nm
s) r) cs SEM -COMPO
80 nm
100 nm
68 nm
100 nm 20nm
10 nm
2 nm
k) l) n)m) cs SEM
u) w) cs SEM -COMPO x)
100 nm 10 nm
126 nm
10 nm
100 nm
a) b) c) cs SEM d)
f) g)
2 1/nm
101
004
200
105/
211
204
215
2 1/nm
2 1/nm
TiO
2
-
anatase
IrO
2
+TiO
2
rutile?
101
004
200
105/211
204
110
101
111/
211
220
2 1/nm
IrO
2
-rutile
110
101
Structural formula of precursor SEM: top view SEM: high resolution SEM: cross section TEM SAEDT
calc.
1 K/min
20 min at
475 °C
1 K/min
20 min at
400 °C
5 min at
375 °C
10 min at
400 °C
(30wt. % Ir)
10 min at
400 °C
(30wt. % Ir)
e)
100 nm
93 nm
h) cs SEM i)
o)
z)
t)
IrO
2
/TiO
2
(Ir(OAc)
3
+TALH)
IrO
2
(Ir(OAc)
3
)
+
TiO
2
(TALH)
TiO
2
(TiCl
4
)
+
IrO
2
/TiO
2
(Ir(OAc)
3
+TiCl
4
)q)
10 nm
v)
10 nm
TiO
2
-anatase
low crystallinity/
amorphous
j) TiO
2
-anatase
2 1/nm
100 nm
y)
100
101
5.1 Influence of precursor on structure/morphology (TiO2, IrO2, IrO2/TiO2)
An overview on the structure of metal oxides of iridium and titanium and mixtures thereof are
provided in Figure 43. The scheme illustrates the morphology and crystallinity of TiO2
synthesized from TiCl4 (a - e), TiO2 synthesized from TALH (f - j), IrO2 synthesized from
Ir(OAc)3 (k - o), IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4 (p - t), as well as IrO2/TiO2
synthesized from Ir(OAc)3 and TALH (u - z).
TiO2 synthesized from TiCl4
The first row shows TiO2 dried for 4 h at 80 °C and calcined at 475 °C (1 K/min). All images
were published by Ortel et al.[98] and are reused with the permission of John Wiley.
Templated mesopores with a spherical shape are visible at the outer surface plane area
(Figure 43 a) suggesting the successful introduction of mesoporosity. SEM images with
higher mangification (Figure 43 b) show a smooth appearance of the pore walls and no sign
of textural porosity. SEM recorded in cross section shows a layer thickness of 126 nm
(Figure 43 c). TEM indicates the presence of mesoporosity suggesting complete pore
penetration of the film volume area (Figure 43 d). The corresponding SAED reveals
diffraction rings and spots that are attributed to a crystalline TiO2-anatase phase. The
synthesis produces layers of mesoporous templated TiO2-anatase with smooth pore walls
TiO2 synthesized from TALH
The second row depicts mesoporous TiO2 dipcoated from a solution of Titanium(IV)
bis(ammonium lactato)dihydroxide (TALH) on silicon substrates and heat treated at 400 °C
(1 K/min). SEM and SAED were published by Ortel et al.[109] and reused with the permission
of ACS. The SEM shows mesoporosity at the outher surface plane area indicating the
introduction of mesoporosity (Figure 43 f). The SEM image obtained in high resolution mode
reveals textural porosity within the mesopore walls (Figure 43 g). Cross section SEM
determines the layer thickness (93 nm, Figure 43 h). The presence of mesoporosity in the
TEM image suggests a complete penetration of the film volume area by mesopores (Figure
43 i). The SAED measurements show diffraction rings associated with a crystalline TiO2-
anatase phase (Figure 43 j). The synthesis approach produces layers of mesoporous
templated TiO2-anatase with pore walls characterized by textural porosity
IrO2 synthesized from Ir(OAc)3 (data from chapter 4.2)
SEM images of templated IrO2 synthesized from Ir(OAc)3 and heat treated at 375 °C are
shown in Figure 43 k. Templated mesoporosity is present at the outer surface plane area.
Higher magnification in SEM reveals textural porosity within the mesopore walls (Figure 43 l).
The layer thickness determined by SEM amounts to 68 nm (Figure 43 m). TEM reveals
102
mesoporosity suggesting that the pores completely penetrate the whole film volume area
(Figure 43 n). Recorded SAED images show broad and weak diffraction rings indicating an
IrO2-rutile phase with a very low crystallite size (Figure 43 o). The synthesis produces layers
of mesoporous templated IrO2-rutile with low crystallinity and textural porosity.
IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4 (data from chapter 4.3)
The fourth row of Figure 43 shows the structural properties for mixed metal oxides of
IrO2/TiO2 obtained by Ir(OAc)3 and TiCl4 heat treated in air at 400 °C. The SEM image shows
templated and untemplated domains (ca. 100 nm in diameter) at the outer surface plane area
(Figure 43 p). SEM micrographs recorded in COMPO mode (Figure 27 b) reveal a higher
brightness for the untemplated than for the templated domain. Hence, the untemplated
domains contain a higher content of iridium, whereas the templated domains contain more
titanium. High resolution SEM reveals textural porosity in the untemplated domains (Figure
43 q), whereas textural porosity is less pronounced in the mesoporous templated titanium
rich domains. The layer thickness was derived by SEM in COMPO mode (95 nm, Figure 43
r). The observed difference in z-contrast in cross section SEM in COMPO mode suggests a
three-dimensional segregation of IrO2 and TiO2. TEM images show mesoporosity suggesting
complete penetration of the film volume area by pores (Figure 43 s). The dark areas
observed in Figure 43 s show a higher brightness for images recorded in HAADF mode
(Figure 27 e) indicating that iridium rich phases are present within the film volume. Recorded
SAED images show no diffraction rings (Figure 43 t) representative for samples with
crystallites too small to produce signals sufficient enough to be detected in SAED. The
synthesis produces layers of mesoporous templated titanium rich and untemplated iridium
rich domains on a lengthscale of ca. 100 nm. Both domains are characterized by low
crystallinity, wheras the iridium rich domain features a high degree of textural porosity.
IrO2/TiO2 synthesized from Ir(OAc)3 and TALH (data from chapter 4.4)
The last row of Figure 43 shows the physicochemical analysis of IrO2/TiO2 synthesized from
Ir(OAc)3 and TALH calcined at 400 °C. The SEM image (Figure 43 u) reveals mesoporosity
at the outer surface plane area. Furthermore, high resolution SEM reveals textural porosity at
the mesopore walls (Figure 43 v). The layer thickness amounts to 80 nm (Figure 43 w). TEM
images recorded in brightfield mode with high magnification (Figure 43 x) reveal small areas
(ca. 2 nm) which appear darker than the surrounding which can be attributed to an iridium
rich domain. The observed mesoporosity (Figure 43 y) suggests complete penetration of the
layer by pores. Recorded SAED images (Figure 43 z) indicate pronounced diffraction rings
attributed to a TiO2-anatase and to a rutile phase. However, similar lattice parameters of IrO2-
rutile, TiO2-rutile, as well as the broadness of reflection rings prevent a clear distinction
between IrO2-rutile, TiO2-rutile, or a mixture thereof, which is noted as: “IrO2+TiO2 rutile?”
103
Figure 44: Influence of calcination temperature (Tcalc.) on the morphology of PEO-PB-PEO templated TiO2 derived by TiCl4 (1st row, silicon substrate, ramp: 1 K/min),
and TALH (2nd row, silicon substrate, ramp: 1 K/min); IrO2 derived by Ir(OAc)3 (3rd row, titanium substrate, preheated furnace); as well as IrO2/TiO2 derived by Ir(OAc)3
and TiCl4 (4th row, titanium substrate, preheated furnace), as well as Ir(OAc)3 and TALH (5th ro w, titanium substrate, preheated furnace).
100 nm 100 nm 100 nm 100 nm
100 nm 100 nm 100 nm 100 nm 100 nm
100 nm 100 nm 100 nm 100 nm 100 nm
100 nm
80 °C
IrO
2
/TiO
2
(Ir(OAc)
3
+TiCl
4
)
IrO
2
/TiO
2
(Ir(OAc)
3
+TALH)
IrO
2
(Ir(OAc)
3
)
+
TiO
2
(TALH)
TiO
2
(TiCl
4
)
+
Structural formula of precursor Tcalc.
1 K/min
20 min at
T
calc.
1 K/min
20 min at
T
calc.
5 min at
T
calc.
10 min at
T
calc.
(30wt. % Ir)
10 min at
T
calc.
(30wt. % Ir)
200 °C 300 °C 400 °C 600 °C500 °C
100 nm 100 nm 100 nm 100 nm 100 nm 100 nm
100 nm100 nm100 nm100 nm100 nm100 nm
c1) 325 °C c3) 550 °C c4) 625 °C
b1) COMPO
a1) COMPO a2) COMPO
d1) COMPO
a3) a4) a5) a6)
b3) b4) b5) b6)b2)
c2)
d3) d4) d5) d6)d2)
e2) e3) e4) e5)e1)
103
104
5.2 Influence of calcination temperature on morphology (TiO2, IrO2, IrO2/TiO2)
Figure 44 shows the influence of calcination temperature on the morphology of TiO2
synthesized from TiCl4 (a1-a6), TiO2 synthesized from TALH (b1 - b6), IrO2 synthesized from
Ir(OAc)3 (c1 - c4), IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4 (d1 - d6), as well as IrO2/TiO2
synthesized from Ir(OAc)3 and TALH (e1 - e5).
TiO2 synthesized from TiCl4
TiO2 obtained by TiCl4 on silicon was dried at 80 °C for 4 h and heat treated between 200 -
600 °C in air (ramp: 1 K/min). A calcination temperature between 80 and 300 °C show a poor
contrast and brightness due to their insufficient electrical conductivity which is most likely
related to an incomplete removal of the polymer template (Figure 44 a1 - a3). An increase in
calcination temperature to 400 and 500 °C (Figure 44 a4 - a5) produces a fully developed
pore system with a smooth appearance of the mesopore walls (see Figure 43 b for higher
resolution). The beginning distortion of the mesopores observed for samples heat treated at
600 °C (Figure 44 a6) indicate ongoing sintering which is induced by crystallite growth.
TiO2 synthesized from TALH
The 2nd row in Figure 44 shows layers of TiO2 obtained by TALH thermally treated at
temperatures between 80 and 600 °C in air (1 K/min). Samples dried at 80 °C show a poor
contrast and brightness in SEM suggesting an incomplete template removal (Figure 44 b1).
However, increasing the calcination temperature to 200 °C produces samples with a good
contrast and brightness due to a developed mesoporous system (Figure 44 b2). The pore
walls have textural porosity (note that textural porosity is more evident in images recorded at
higher magnification, e.g. Figure 43 g). A further increase in calcination temperature to 300
and 400 °C show no significant change of the mesopore shape or textural porosity at the
outer surface plane area (Figure 44 b3 - b4). Grains and a beginning distortion of the
spherical mesoporous shape can be observed for samples heat treated at 500 °C (Figure 44
b5). In addition, textural porosity starts to decline. If the calcination temperature is further
increased to 600 °C, not only a higher degree of distortion of the spherical mesoporous
shape is occuring, but also an almost complete depletion of textural porosity (Figure 44 b6).
Both observations are attributed to the ongoing sintering due to temperature induced
crystallite growth.
IrO2 synthesized from Ir(OAc)3
Layers of mesoporous templated IrO2 were obtained by Ir(OAc)3 and a subsequent heat
treatment at temperatures between 325 and 625 °C. Thermally prepared IrO2 at 325 °C
shows a poor contrast and brightness in SEM indicating incomplete polymer template
105
removal (Figure 44 c1). An increase in calcination temperature to 400 °C (Figure 44 c2)
reveals a fully developed pore system with additional textural porosity in the mesopore walls
(see Figure 43 l for SEM with higher magnification). Heat treated samples between 550 and
625 °C (Figure 44 c3 - c4) show a beginning distortion of mesopore walls and an almost fully
depletion of textural porosity caused by temperature induced crystallite growth.
IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4
IrO2/TiO2 was coated on titanium and obtained by different metal oxide precursors, such as
Ir(OAc)3 and TiCl4. The samples were heat treated at temperatures between 80 and 600 °C.
Low calcination temperatures between 80 and 300 °C (Figure 44 d1 - d3) show largely
segregated areas with a high content of iridium and titanium, respectively. Moreover, a poor
contrast and brightness is observed suggesting incomplete polymer template removal.
Enhancing the calcination temperature to 400 °C (Figure 44 d4) reveals a templated, titanium
rich domain as well as an untemplated, iridium rich domain (suggested by COMPO Figure 27
b). The untemplated areas are rich in textural porosity, whereas templated areas show less
degree of textural porosity (see Figure 43 q). A heat treatment of samples at 500 and 600 °C
(Figure 44 d5 - d6) is accompanied by a depletion of textural porosity and a formation of
bright particles suggesting temperature induced crystallite growth.
IrO2/TiO2 synthesized from Ir(OAc)3 and TALH
Ir(OAc)3 and TALH served as metal oxide precursors for the preparation of IrO2/TiO2 on
titanium substrates. The samples were calcined at temperatures between 200 and 600 °C.
Samples heat treated between 200 and 300 °C (Figure 44 e1 - e2) show a poor contrast and
brightness suggesting an incomplete polymer template removal. A fully developed pore
system with an additional content of textural porosity is observed for samples heat treated at
400 °C (Figure 44 e3 and Figure 43 v). A further increase in calcination temperature to 500
and 600 °C reveals particles arising on the outer surface plane area (Figure 44 e4 - e5). The
temperature induced demixing is caused by the excessively crystallisation behaviour of IrO2.
106
Figure 45: A general scheme based on the observations from Figure 44 (Influence of precursor on morphology) and Figure 43 (influence of calcination temperature on
morphology/crystallinity). The figure depicts the structural formula of the utilized precursors; the corresponding equilibrated solutions; the morphology of films
deposited on a substrate and dried at 80 °C; and the morphology/crystallinity after heat treatment at temperatures between 200 - 600 °C.
TiCl
4
fast
PEO-PB-PEO
Ethanol + H
2
O
Equilibrated
solution
Ingredients
TALH none
PEO-PB-PEO
Methanol + H
2
O
TALH none
Ir(OAc)
3
none
PEO-PB-PEO
Methanol + H
2
O
TiCl
4
fast
Ir(OAc)
3
none
PEO-PB-PEO
Ethanol + H
2
O
Ir(OAc)
3
none
PEO-PB-PEO
Ethanol + H
2
O
Mesophase
formation
Drying 80 °C Densi-
fication
Hydrolysis +
condensation
rate
TiO
2
anatase
Ir rich
phase
Ti rich
phase
titanium
silicon
TiO
2
anatase
silicon
TiO
2
anatase
silicon
silicon
Ti rich
phase
titanium
Ir rich
phase
titanium
titanium
ca. 200 °C
-300 °C
ca. 350 °C
-450 °C
ca. 500 °C
-600 °C
Ti rich
rutile
Ir rich
rutile
titanium
TiO
2
anatase
titanium
titanium
titanium
Thermal treatment in airFilm depositionEducts and properties
IrO
2
rutile
(low crystallinity)
titaniumtitanium
IrO
2
rutile
titaniumtitanium
+
+
Structural formula of precursor
TiO
2
anatase
silicon
TiO
2
anatase
silicon
silicon
4 h
80 °C
4 h
80 °C 1 K/min
or
20 min
@ T
calc.
80 °C
10 min
10 min
80 °C
@ T
calc.
5 min
@ T
calc.
10 min
@ T
calc.
80 °C
10 min
10 min
1 K/min
20 min
@ T
calc.
Low crystallinity
Low crystallinity,
mixed rutile ?
Textural
porosity
Textural
porosity
Textural
porosity
Textural
porosity
IrO
2
/TiO
2
(Ir(OAc)
3
+TiCl
4
)
IrO
2
/TiO
2
(Ir(OAc)
3
+TALH)
IrO
2
(Ir(OAc)
3
)
TiO
2
(TALH)
TiO
2
(TiCl
4
)TiCl
4-x-y
(OEt)
x
(OH)
y
TiCl
4-x-y
(OEt)
x
(OH)
y
Ageing
80 °C
or
or
or
Ir rich
rutile
Ti rich
rutile
silicon
Low crystallinity Textural
porosity
106
107
5.3 Processes during synthesis and the resulting morphology
Figure 45 combines the observations from chapter 5.1 and 5.2 in a general scheme in order
to illustrate processes occuring during the preparation of dipcoating solutions, film deposition,
and subsequent heat treatments for TiO2 synthesized from TiCl4 (1st row), TiO2 synthesized
from TALH (2nd row), IrO2 synthesized from Ir(OAc)3 (3rd row), IrO2/TiO2 synthesized from
Ir(OAc)3 and TiCl4 (4th row), and IrO2/TiO2 synthesized from Ir(OAc)3 and TALH (5th row).
TiO2 synthesized from TiCl4 (1st row)
Titanium tetrachloride is often used to obtain nanostructured TiO2 (see chapter 2.2.6). In
literature, it is reported that TiCl4 shows fast hydrolysis and condensation rates.[99, 102]
However, hydrolysis and condensation of TiCl4 produces HCl which prevents further
polycondensation and therefore leads to the formation of self stabilized titanium oligomers
with particle diameters in the range of 0.4 - 1.7 nm.[107] Figure 45 (1st row) depicts the
equilibrated solution of TiCl4 dissolved in ethanol, water and PEO-PB-PEO. The obtained
titanium oligomers are shown as small spherical particles well dispersed in the solvent.
Moreover, these oligomers are typically terminated by hydroxide groups thus possessing the
capability to interact with hydrolytic regions of the utilized polymer, e.g. PEO.[99, 102]
Subsequent to dipcoating, the solvent evaporates together with HCl triggering two effects: i)
the alignment of pre formed micelles and ii) a further polycondensation of the titanium
oligomers.[157] The obtained samples are dried for 4 h at 80 °C (ensuring reproducibility[99])
and are further heat treated at temperatures above 400 °C in air to fully remove the polymer
template and to convert the precursor into a crystalline TiO2-anatase with smooth pore walls.
This pore wall structure was already reported in literature[98] and is associated with highly
crystalline materials. This assumption is in good agreement with XRD of the corresponding
samples calcined at 400 °C. The Scherrer equation applied at the (101) reflection reveals a
crystallite size of ~20 nm. An increase of calcination temperatures to 500 and 600 °C further
enhances the crystallite size to 21 and 23 nm which distort the spherical mesopore shape.
TiO2 synthesized from TALH (2nd row)
Titanium(IV) bis(ammonium lactato)dihydroxide (abbreviated as: TALH) is characterized by a
Ti cation complexed by lactic acid (chelat ligand), and two hydroxide groups. Chelat groups
show rather slow hydrolysis rates compared to alkoxy groups.[158] In fact, TALH does not
undergo hydrolysis and condensation when dissolved in water.[149] The graphical illustration
of the equilibrated solution (Figure 45; 2nd row) thus depicts a particle character only for PEO-
PB-PEO polymer templates, whereas TALH does not form any particles (in contrast to TiCl4).
Calcination at 200 °C shows mesoporosity and textural porosity. The successful preparation
of mesoporous TiO2 by using TALH demonstrates, that precursors without hydrolysis and
108
condensation capabilities can be used along with polymer templates in order to successfully
synthesize mesoporous samples. The occuring textural porosity for TiO2 obtained by TALH
and the presence of smooth pore walls for TiO2 derived by TiCl4 suggests that the carbon
content of the precursor significantly changes the microstructure of the mesopore walls. The
decomposition of carbon containing precursors forms CO2 during calcination. Hence, a
possible explanation for the textural porosity might be the departure of CO2 during heat
treatment. This observation is in line with reports of Schmack et al.[148] who observed a clear
correlation between the carbon content in metal oxide precursors and degree of textural
porosity in the mesopore walls of templated films. The corresponding XRD for samples
calcined at 400 °C reveal a crystallite size of ca. 4 - 5 nm (Scherrer equation, (101) reflection,
Figure A4 a). The lower crystallite size for TALH based TiO2 films (4 - 5 nm, Figure A4 b) in
comparison to TiCl4 based TiO2 films (20 nm) can be attributed to the higher carbon fraction
of the TALH precursor which potentially inhibits temperature induced crystallite growth. The
degree of textural porosity declines as a function of calcination temperature. Moreover, the
distortion of the spherical mesopore shape depends on the applied temperature during heat
treatment. A depletion of the textural porosity and distortion of the mesopore shape are due
to sintering which is induced by ongoing crystallite growth.
IrO2 synthesized from Ir(OAc)3 (3rd row)
Ir(OAc)3 is stable to hydrolysis and condensation in water and ethanol at room
temperature,[145] forms no small oligomers and is therefore chemically similar to TALH.
Dissolving PEO-PB-PEO and Ir(OAc)3 in ethanol and water forms a clear greenish solution
(Figure 45; 3rd row). Thermal treatment of deposited layers between 80 and 300 °C in air
does not fully remove the polymer. However, a fully developed pore system is obtained when
heat treating at 400 °C. The mesopore walls contain textural porosity (see Figure 43 l) as it
was the case for TiO2 obtained by TALH. As to the similar chemical behaviour of Ir(OAc)3
and TALH comparable morphologies of the obtained mesoporous layers are obtained. The
textural porosity might be explained by the formation of CO2 as the metal oxide precursor
decomposes during thermal treatment.[148] An increase in calcination temperature leads to a
depletion of textural porosity and distortion of the spherical mesopore shape indicating
ongoing sintering due temperature induced crystallite gowth.
IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4 (4th row)
In order to produce mixed metal oxides of Ti and Ir, Ir(OAc)3 and TiCl4 were immersed in
ethanol and water. Ir(OAc)3 was found to be stable against hydrolysis and condensation,[145]
and thus showing a poor interaction with hydrolytic regions of the polymer template, whereas
TiCl4 shows fast hydrolysis and condensation rates and can interact with the polymer.
109
The equilibrated solution of TiCl4, Ir(OAc)3, PEO-PB-PEO, ethanol, and water (Figure 45; 4th
row) is characterized by small titanium oligomers, PEO-PB-PEO micelles and Ir(OAc)3
dissolved in ethanol and water. The solution was light green and clear indicating that no light
is scattered by particles that are dispersed within the suspension. The Tyndall effect usually
occurs for particles dispersed in a liquid medium with a diameter of at least ~100 nm.[146-147]
As a consequence, the produced solution is not expected to contain particles exhibiting
diameters larger than ca. 100 nm. However, dipcoating on titanium with a subsequent heat
treatment at 80 °C reveals largely segregated domains with diameters of at least 100 nm. An
increase in calcination temperature to 400 °C removes most of the polymer template and
reveals an untemplated, iridium rich domain with textural porosity and a templated, titanium
rich domain with less textural porosity. A further increase in calcination temperature
diminishes the textural porosity, and forms particles, whereby the spherical mesoporous
shape distorts under the development of an Ir rich and Ti rich rutile phase
Three important effects are observed: i) the segregation of IrO2 and TiO2 on a lengthscale of
roughly 100 nm, ii) the development of a mesoporous structure solely for titanium rich
domains and iii) a higher degree of textural porosity for iridium rich domains. i) The
synthesized dipcoating solution contains PEO-PB-PEO, TiCl4 and Ir(OAc)3 in ethanol and
water, was clear and showed a greenish colour. Therefore, as particles with a diameter of
larger than ~100 nm are not present in the solution,[146-147] the observed segregated domains
in the layers are not formed within the solution. Thus, demixing very likely occurs after film
deposition and is possibly related to different drying behaviours of Ir and Ti precursors. The
distinct behaviours might be associated with different mobilities of both metal oxide
precursors within the solution. We hypothesize that the different mobilities are related to the
different interaction behaviours: TiCl4 interacts with the polymer template, whereas Ir(OAc)3
does not. Moreover, the different interaction behaviours of TiCl4 and Ir(OAc)3 with the
polymer template are used to describe ii) the development of mesoporosity solely for titanium
rich domains. It appears likely to find a precursor molecule next to a polymer molecule if the
precursor is able to interact with the polymer (e.g. TiCl4). As a consequence, Ti rich domains
appear to be mesoporous templated, whereas iridium rich domains show no sign of
templated mesoporosity. However, the iii) iridium rich domains exhibit a high degree of
textural porosity in contrast to the templated Ti rich domains. This behaviour is associated
with the higher degree of carbon within Ir(OAc)3 than TiCl4. During calcination the carbon
oxidizes to CO2, whereby textural porosity is introduced to the iridium rich domains.[65, 148]
IrO2/TiO2 synthesized from Ir(OAc)3 and TALH
Both, Ir(OAc)3 and TALH are characterized by sterically demanding chelat ligands, such as
acetic acid and lactic acid, respectively. Hence, no hydrolysis and condensation is observed
110
to form hydroxide groups which prevents the interaction with the polymer template. The
obtained dipcoating solution of PEO-PB-PEO, Ir(OAc)3 and TALH in methanol showed a
green colour without turbidity.
A layer deposited on titanium substrate was heat treated at 200 °C and showed i) a poor
contrast and brightness in SEM suggesting incomplete template removal and ii) no largely
segregated areas with diameters of 100 nm as it was observed in the case of TiCl4 and
Ir(OAc)3. A more even distribution of IrO2 and TiO2 after film deposition might be related to a
similar drying behavior of Ir(OAc)3 and TALH. Both metal oxide precursors therefore show
similar, however no attractive, interactions with the polymer template. We hypothesize, that
higher chemical similarity of the used metal oxide precursors result in a more homogenous
distribution of IrO2 and TiO2 within films. An increase to 400 °C features a fully developed
pore system (Figure 44) with textural porosity in the mesopore walls due to the combustion of
carbon to CO2 from both used metal oxide precursors. However, TEM studies show small
(ca. 2 nm) segregated and dark areas in brightfield mode suggesting a higher amount of Ir
than Ti. According to SAED images, TiO2-anatase and rutile are present. Due to the
broadness of the rings and the similar lattice parameters of TiO2-rutile and IrO2-rutile, a clear
distinction between both rutile phases (IrO2 and TiO2) or a mixture thereof can not be given.
Therefore, the presented scheme in Figure 45 (5th row) shows i) TiO2 anatase, ii) small Ir rich
domains, and iii) titanium rich domains, whereof, ii) and iii) are possibly crystallized in a rutile
structure. Further increasing the calcination temperature, not only distort the spherical
mesopore shape but also forms iridium rich crystallites (Figure 34 a). XRD (Figure 34 b, c)
shows distinct reflection signals corresponding to TiO2 anatase, TiO2 rutile containing Ir (Ti-
rich rutile), and IrO2 rutile containing Ti (Ir-rich rutile). Obviously, two effects are observed: i)
a thermally induced demixing, and ii) the beginning formation of a solid solution.
Tammann[150] reported, that atoms can change places within crystallites or at the interface
between two different crystallite species, if a sufficient degree of atomic oscillation
(temperature dependent) is reached. In honour of Tammann, this temperature is called the
Tammann temperature. The Tammann temperatures for TiO2 and IrO2 are as followed:
TiO2: TTammann = 791 °C[151]
IrO2: TTammann = 413 °C[152]
i) For IrO2 the lower Tammann temperature implies mobility at much lower temperatures than
required for TiO2. Hence, thermally induced demixing of IrO2/TiO2 slowly begins for samples
calcined above ca. 400 °C. In fact, for samples calcined at 400 °C a demixing between IrO2
and TiO2 is not very pronounced, whereas samples heat treated at 500 °C clearly depict
larger areas with Ir rich crystallites. ii) A further increase in calcination temperature to 600 °C
forms a solid solution of IrO2 and TiO2. We assume, that present IrO2 crystallites starts to
incorporate surrounded TiO2 leading to fractions of Ir rich rutile and titanium rich rutile.
111
5.4 Influence of calcination temperature on OER activity and ECSA
In dependency of the calcination temperature, the following chapter shows the quantified
electrochemical measurements of the oxygen evolution reaction (OER) activity and the
electrochemical accessible surface area (ECSA) of mesoporous templated IrO2 and
IrO2/TiO2, respectively. The electrochemical data are then related to the morphology. Figure
46 shows for IrO2 and IrO2/TiO2 (synthesized from TiCl4 or TALH) the a) OER activity and b)
corresponding ECSA as a function of calcination temperature, as well as the c) OER activity
as a function of ECSA.
Figure 46: Influence of calcination temperature on a) OER activity and b) corresponding ECSA. Moreover
the c) OER activity is plotted as a function of ECSA. IrO2 (black) was synthesized from Ir(OAc)3 and heat
treated for 5 min at Tcalc.; IrO2/TiO2 (purple) was synthesized from Ir(OAc)3 and TiCl4, exhibits a loading of
30 wt. % Ir in Ir/TiO2 and was heat treated for 10 min at Tcalc.; IrO2/TiO2 (green) synthesized from Ir(OAc)3
and TALH with a loading of 30 wt. % Ir in Ir/TiO2 and heat treatment for 10 min at Tcalc.
A comparison of OER activities in dependence of the calcination temperature was
established by measuring the current density at a potential of 1.55 VRHE from the upscan of
the 2nd iR corrected CV (Figure 46 a, note: y-axis is shown logarithmically). The OER activity
is normalized to the substrate’s planar geometrical surface area. Catalytic layers containing
mesoporous IrO2 depict an increase in OER activity in the temperature range of 325 –
375 °C. For higher calcination temperatures the OER activity steadily decreases. From TiCl4
and TALH produced samples display a very similar trend. First, the OER activity is steadily
enhanced in the temperature range between 200 to 400 °C, but successively decreases
between 400 and 600 °C.
Figure 46 b shows the quantified ECSA measurements of the corresponding samples from
Figure 46 a. The ECSA (in Coloumb) is obtained by the mean value of the integrated anodic
and cathodic charge from CVs recorded in a lower potential window between 0.40 –
1.40 VRHE. The ECSA follows a very similar trend as the OER activity in dependency of
temperature. The IrO2 ECSA successively increases up to temperatures as high as 375 °C
200 300 400 500 600
0.01
0.1
1
10
100
j at 1.55 V vs. RHE / mA cm
-2
geo
T
calc.
/ °C
200 300 400 500 600
10-5
10-4
10-3
10-2
ECSA / C
T
calc.
/ °C
10
-5
10
-4
10
-3
10
-2
0.01
0.1
1
10
100
j at 1.55 V vs. RHE / mA cm
-2
geo
ECSA / C
Ir(OAc)
3
+ TALH
Ir(OAc)
3
+ TiCl
4
IrO
2
Ir(OAc)
3
+ TiCl
4
IrO
2
incomplete
template
removal
ongoing
sintering
high
OER
activity
Ir(OAc)
3
+ TALH
Ir(OAc)
3
+ TALH
IrO
2
incomplete
template
removal
ongoing
sintering
high
surface
area
incomplete
template removal
(T
calc
< 325 °C)
current density
scales with ECSA
(T
calc
> 350 °C)
Ir(OAc)
3
+ TiCl
4
a) OER activity vs. T
calc.
b) ECSA vs. T
calc.
c) OER activity vs. ECSA
112
and progressively declines for higher calcination temperatures. The ECSA of IrO2/TiO2 either
synthesized from TiCl4 or TALH follow a very similar trend as a function of calcination
temperature. An increase in ECSA is observed for both systems between 200 and 400 °C,
but subsequently declines with respect to the calcination temperature. In Figure 46 c the
influence of the ECSA on the OER activity is established for each system. Samples heat
treated below 325 °C show a poor OER activity and a small ECSA, whereas samples
calcined at temperatures higher than 350 °C depict a higher OER activity and a larger ECSA
with a fairly linear relationship.
Based on the present data the following conclusion is drawn. All samples that were thermally
treated between 200 and 325 °C show an incomplete removal of the polymer template
(Figure 44) which blocks the mesopores and consequently causes a small ECSA. An
increase of calcination temperature slightly higher than the combustion temperature of the
polymer template (350 – 475 °C) produces low crystallinity (Figure 43) and a fully accessible
pore system as indicated by Kr-physisorption (Figure 23 b). A high surface area is the
consequence. The depletion of textural porosity and distortion of mesopores is induced by a
further increase in calcination temperature (> 500 °C) and progressively decreases the
ECSA. The loss in porosity related to an ongoing sintering is caused by thermally induced
crystallite growth (Figure 44 (SEM of IrO2 and IrO2/TiO2), Figure 24 (XRD of IrO2), Figure 28
(XRD of IrO2/TiO2, TiCl4), Figure 34 (XRD of IrO2/TiO2, TALH)). In conclusion, temperatures
slightly higher than the decomposition temperature of the polymer template produce samples
with a high surface area. Moreover, if the polymer is removed, a fairly linear relationship
between the OER activity and ECSA is observed suggesting that ECSA contributes to the
OER activity.
5.5 Influence of crystallinity on OER activity
The degree of crystallinity influences the intrinsic OER reactivity of mesoporous IrO2 as
described in chapter 4.2.4. It was observed that IrO2 heat treated at or temperatures higher
than 550 °C display crystallites large enough to produce distinct diffraction signals in XRD. At
lower calcination temperatures, however, no XRD reflections are observed but very broad
diffraction rings in SAED images due to low crystallinity (Figure 24). Furthermore, samples
with a low crystallinity show higher intrinsic OER reactivity (Figure 23).
As thermally treated IrO2/TiO2 (synthesized from Ir(OAc)3 and TiCl4) at 400 °C show no
significant diffraction rings in SAED (Figure 43, 4th row) the obtained layer is composed of
crystallites too small in size to produce intense reflections. The reflections in XRD at 500 °C
can be attributed to a Ti rich rutile and an Ir rich rutile phase (Figure 28).
113
A heat treatment at 400 °C of IrO2/TiO2 synthesized from Ir(OAc)3 and TALH show rings in
SAED images corresponding to TiO2 anatase, and rutile (Figure 43). However, no distinct
reflections have been observed in XRD diffraction patterns (Figure 34 b). At calcination
temperatures higher than 500 °C diffraction patterns of a TiO2 anatase, a Ti rich rutile, and a
iridium rich rutile phase are observed (Figure 34 b).
In order to reveal the impact of crystallinity on the OER activity different criteria for
crystallinity have to be defined. A sample is considered as i) low crystalline, if no distinct
reflections are observed in XRD but diffraction rings in SAED. And it is considered as ii) high
crystalline, if distinct reflections are shown in XRD. For samples with a removed template
Figure 47 depicts the measured OER activity during the upscan of the 2nd iR corrected CV at
a potential of 1.55 VRHE as a function of crystallinity for a) IrO2, b) IrO2/TiO2 (synthesized from
Ir(OAc)3 and TiCl4), and c) IrO2/TiO2 (synthesized from Ir(OAc)3 and TALH).
Figure 47: Influence of crystallinity on the OER activity from catalytic layers coated on titanium
substrates. Three different systems are shown for comparison: a) IrO2, b) IrO2/TiO2 synthesized from
Ir(OAc)3 and TiCl4, as well as c) IrO2/TiO2 synthesized from Ir(OAc)3 and TALH. The OER activity was
accessed by measuring the current density (with respect to the planar geometrical surface area) in the
upscan of the 2nd iR corrected CV at potentials of 1.55 VRHE (1600 rpm, 6 mV/s, 0.5 M H2SO4).
Figure 47 a reveals the OER activity for IrO2 with low crystallinity (3 bars on the left side, Tcalc.
= 375, 400, 475 °C) and high crystallinity (2 bars on the right side, Tcalc. = 550, 625 °C). In
Figure 47 b the OER activity of IrO2/TiO2 (TiCl4) is shown for low cystallinity (1 bar on the left
side, Tcalc. = 400 °C) and high crystallinity (2 bars on the right side, Tcalc. = 500, 600 °C).
Finally, Figure 47 c depicts the OER activity of IrO2/TiO2 (TALH) with low crystallinity (1 bar
on the left side, Tcalc. = 400 °C) and high crystallinity (2 bars on the right side, Tcalc. = 500,
600 °C).
It is obvious, that materials with a lower degree of crystallinity exhibit a higher OER activity
which is in line with the observations made for mesoporous templated IrO2 in chapter 4.2.4. A
high calcination temperature leads to an increase in crystallite size and a decrease in ECSA.
It was shown, that ECSA exhibits a severe impact on the OER activity (Figure 46 c).
Therefore, the decrease in the OER activity shown in Figure 47 is not solely related to the
0.01
0.1
1
10
100
j at 1.55 V vs. RHE / mA cm
-2
geo
a) IrO
2
(Ir(OAc)
3
)
b) IrO
2
/ TiO
2
(Ir(OAc)
3
+TiCl
4
)
c) IrO
2
/ TiO
2
(Ir(OAc)
3
+TALH)
low
crystallinity
(SAED rings)
high
crystallinity
(XRD reflections)
low
crystallinity
(SAED rings)
high
crystallinity
(XRD reflections)
low
crystallinity
(SAED rings)
high
crystallinity
(XRD reflections)
114
change of crystallinity as both, the crystallinity and the ECSA are strongly affected by the
applied calcination temperature. Consequently, Figure 47 shows the overlapping influences
of a decreasing surface area and an increasing crystallinity on the OER activity of IrO2 and
IrO2/TiO2.
For this reason, it appears difficult to investigate mesoporous IrO2 and IrO2/TiO2 with the
same active surface area but a different crystallinity. In order to study the influence of ECSA
on the OER activity independent of crystallinity, chapter 5.6 shows a variation of the IrO2
content in TiO2 calcined at similar temperatures, whereas chapter 5.7 presents an equal heat
treated IrO2 with different layer thickness.
5.6 Influence of electrical conductivity on OER activity
The electrical conductivity can have a tremendous impact on electrons travelling through the
catalytic layer, to or away, from active centres. The electron transport is hindered if, for
instance, an insufficient degree of electrical conductivity is present, thus causing an
additional overpotential in electro catalytic reactions such as the oxygen evolution reaction.
The additional overpotential during electrochemical testing is shown for IrO2/TiO2 with low
iridium loading produced from Ir(OAc)3 and TALH (chapter 4.4). The electrical conductivity of
IrO2/TiO2 showed a significant increase if a certain amount of conductive iridium is added.
This behaviour is in fair good agreement with percolation theory[74, 77] describing the electrical
conductivity of randomly packed conductive and insulation particles. A more comprehensive
illustration across more systems on the impact of electrical conductivity on intrinsic reactivity
is depicted in Figure 48.
Figure 48 shows the OER activity as a function of ECSA for IrO2/TiO2 (Ir(OAc)3+TALH,
400 °C) with iridium loadings between a) 0 to 100 wt. % Ir in Ir/TiO2 and b) 0 to 25 wt. % Ir in
Ir/TiO2. Furthermore, c) depicts the OER activity plotted as a function of electrical
conductivity. In order to identify general trends d) shows the OER activity of IrO2/TiO2
(synthesized from Ir(OAc)3, and TiCl4 or TALH, respectively) for different iridium loadings
calcined at 400 °C, for different calcination temperatures with an iridium loading of 30 wt. % Ir
in Ir/TiO2.
115
Figure 48: Infuence of a, b) ECSA and c, d) sheet conductivity on the OER activity. For IrO2/TiO2
(produced from Ir(OAc)3 and TALH) the a) OER activity scales linearly in the region of 30 - 100 wt. % Ir.
However, a discrepancy from the linear relationship is observed at b) lower loadings of Ir in Ir/TiO2. c) The
OER activity further seems to be affected by the electrical sheet conductivity. d) Two regimes are clearly
identified if further data points of Ir(OAc)3 + TiCl4 are added.
Figure 48 a shows the OER activity at 1.60 VRHE as a function of ECSA. A linear dependency
is present between the OER activity and ECSA for iridium loadings between 30 - 100 wt. % Ir
in Ir/TiO2. However, Figure 48 b reveals a discrepancy from the linear fit for samples with
loadings between 5 - 25 wt. % Ir in Ir/TiO2. The observed current density is smaller than
suggested by the extrapolated linear fit of the 30 - 100 wt. % Ir region.
Figure 48 c depicts as a function of electrical sheet conductivity, the OER activity of IrO2
calcined at 375 °C (50 nm, noted as 100 wt. % Ir in Ir/TiO2), IrO2/TiO2 synthesized from
Ir(OAc)3 + TALH calcined at 400 °C with loadings between 0 - 75 wt. % Ir and loadings of
30 wt. % Ir calcined between 200 - 600 °C, respectively. The sheet conductivity was
determined by a sheet resistivity measurement of IrO2/TiO2 on insulating glass substrates
(microscope slides). The values are not corrected for layer thickness. However, systems
obtained under these synthesis conditions typically exhibit layer thicknesses between 50 and
100 nm. Hence, the small difference in layer thickness does not affect the observed
relationships as the x-axis is depicted logarithmically. It is clear to see that the observed OER
10
-15
10
-13
10
-11
10
-9
10
-7
10
-5
10
-3
10
-1
0
10
20
30
40
50
60
70
80
j at 1.60 V vs. RHE / mA cm
-2
geo
Sheet conductivity / Ohm
-1
sq
0.0 2.0x10
-3
4.0x10
-3
0
10
20
30
40
50
60
70
80
j at 1.60 V vs. RHE / mA cm
-2
geo
ECSA / C
10
-15
10
-13
10
-11
10
-9
10
-7
10
-5
10
-3
10
-1
0
10
20
30
40
50
60
70
80
j at 1.60 V vs. RHE / mA cm
-2
geo
Sheet conductivity / Ohm
-1
sq
Ir(OAc)
3
+TALH
Ir(OAc)
3
+TiCl
4
IrO
2
low
OER activity
high
OER activity
d) OER activity vs.
sheet conductivity
Ir(OAc)
3
+TALH
IrO
2
a) OER activity vs. ECSA
(0 -100 wt% Ir)
c) OER activity vs.
sheet conductivity
100 wt%Ir
75
60
45
30
25
20
IrO
2
0.0 2.0x10
-4
4.0x10
-4
0
1
2
3
4
j at 1.60 V vs. RHE / mA cm
-2
geo
ECSA / C
10
0-5
15
20
25 wt.% Ir
b) OER activity vs. ECSA
(0 -25 wt % Ir)
low
OER activity
high
OER activity
20x10
-4
40x 10
-4
116
activity is low until the sheet conductivity reaches values of ca. 10-8 (Ohm/sq)-1. For samples
with higher values, the OER activity seems to be dependent on the electrical conductivity.
In order to provide a comprehensive comparison, Figure 48 d contains in addition to Figure
48 c data points from IrO2/TiO2 synthesized from Ir(OAc)3 + TiCl4 calcined at 400 °C with
loadings between 15 - 75 wt. % Ir and loadings of 30 wt. % Ir calcined between 200 - 600 °C,
respectively. These data points reveal the presence of two regimes i) a low OER activity for
samples with a conductivity below ca. 10-8 (Ohm/sq)-1, and ii) a high OER activity for samples
with values exceeding ca. 10-8 (Ohm/sq)-1.
The present data lead to the following thoughts. The iridium content is an important
parameter that influences the electrical conductivity (Figure 31 b, Figure 37 b). Samples with
a low amount of iridium oxide show a low electrical conductivity which might be insufficient,
thus not providing a fast electron transport through the layer. In order to underline this
assumption, measurements regarding the electron transport were conducted for IrO2/TiO2
with different iridium loadings in the ECSA regime between 0.40 - 1.40 VRHE (Figure 38 c).
The pronounced oxidation and reduction waves were assigned to the IrIII/IrIV redox couple.
The redox waves of samples with lower iridium loadings were far off the equilibrium potential
(Figure 38 b), indicating an insufficient degree of electrical conductivity. Usually, an
insufficient electrical conductivity causes an additional overpotential that most likely affects
the intrinsic reactivity of active iridium centres. The number of active Ir centres (e.g. wt. % Ir
in Ir/TiO2) scale linear with the ECSA. Moreover, the ECSA should exhibit a linear
relationship with the OER activity. If any other process than the surface reaction, such as gas
transport through the pore system or electron conduction to the active site, was the limiting
step, a deviation from the linear behavior would be expected. Samples of IrO2/TiO2 with high
Ir loadings (> 30 wt. % Ir) show a linear dependency between the OER activity and ECSA at
relatively high current densities (ca. 60 mA/cm²), thus excluding transport limitation effects
(Figure 48 a). However, loadings lower than 30 wt. % Ir in Ir/TiO2 show a discrepancy from
the extrapolated linear fit for the higher iridium loading regime suggesting an insufficient
degree of conductivity (Figure 48 b). A hindered electron transport through the layer can be
assumed which causes the reduction of the intrinsic reactivity of active iridium centres.
An increase in Ir content leads to a higher sheet conductivity (Figure 31 b, Figure 37 b),
higher ECSA (Figure 38 c, Figure 48 a), and higher OER activity (Figure 39 b, Figure 48 a).
However, the linear dependency of OER activity and ECSA is still observed with increasing
sheet conductivity (Figure 48 a and c). This suggests that samples with loadings of at least
30 wt. % Ir in Ir/TiO2 and/or a sheet conductivity higher than approximately 10-8 (Ohm/sq)-1
(ca. 0.1 S/m) do not suffer from an additional voltage drop over the layer. If a sufficient
electrical conductivity is provided, the OER activity linearly scales with the ECSA and
ensures the same intrinsic reactivity for active Ir centres dispersed in TiO2 as for “pure” IrO2.
117
5.7 Influence of layer thickness on gas removal rate
The active surface area is expected to scale linear with the amount of active sites, whereas
the amount of active sites can be adjusted with, e.g. the iridium loading in TiO2 (Figure 48 a)
or the layer thickness of a homogenous prepared catalytic layer (this chapter). A deviation of
the linear dependency between OER activity and ECSA at higher geometrical current
densities is therefore associated with a sign of transport limitation of produced O2 within the
pore system. In order to investigate transport limitations mesoporous templated layers of IrO2
coated on titanium cylinders were used as a model system. Different layer thicknesses
between 50 - 225 nm were obtained by dipcoating at withdrawal rates between 10 and
150 mm/min, respectively. Thicker layers could not be obtained with single layer dipcoating
since peeling off from the substrate occured. To solve this problem, multi-layer dipcoating
was used. 4 single layers on titanium substrate were deposited at a withdrawal rate of
30 mm/min and intermediate calcination steps at 200 °C followed by a final heat treatment for
5 min at 375 °C. The layer thicknesses of the corresponding samples were obtained by SEM
(Figure 25 a). Figure 49 shows as a function of layer thickness the a) OER activity and b)
ECSA. In order to identify if transport limitation is present the c) OER activity is shown as a
function of ECSA. For different layer thicknessses the d) Tafel plots, e) kink potentials and
the f) corresponding Tafel slopes are evaluated.
Figure 49: Single layer and multi layer dipcoating techniques were applied in order to obtain mesoporous
IrO2 with different layer thicknesses. The influence of layer thickness is depicted on a) OER activity and b)
ECSA. To investigate the gas removal within the pore system c) the OER activity is plotted as a function
of ECSA. Kinetical aspects are studied by interpreting the d) Tafel plots in terms of e) kink potential and f)
Tafel slopes.
036912 15 18 21 24
0
10
20
30
40
50
60
70
80
90
100
j at different potentials
vs. RHE / mA cm
-2
ECSA / mC
0100 200 300 400 500
0
5
10
15
20
ECSA / mC
Layer thickness / nm
0100 200 300 400 500
0
10
20
30
40
50
60
70
80
90
100
j at 1.55 V vs. RHE / mA cm
-2
geo
Layer thickness / nm
-1.5-1.0 -0.5 0.0 0.5 1.0 1.5 2.0 2.5
1.40
1.45
1.50
1.55
1.60
1.65
1.70
E vs. RHE / V
log j / mA cm
-2
geo
a) OER vs. layerthickness
single layer multi layer
b) ECSA vs. layer thickness
1.50 V
1.53 V
1.55 V
multi layersingle layer
c) OER activity vs. ECSA
480 nm
225 nm
170 nm
120 nm
50 nm
0100 200 300 400 500 600
0
50
100
150
200
250
Tafel slope / mV dec
-1
Layer thickness / nm
f) Tafel slope vs. layer
thickness of IrO2
d) Tafel plots: IrO2
(different layerthickness)
single layer multi layer
e) Kink potential vs. layer
thickness of IrO2
0100 200 300 400 500 600
1.40
1.45
1.50
1.55
1.60
1.65
1.70
Kink potential E vs. RHE / V
Layer thickness / nm
„kink“
118
The OER activity of IrO2 coated on titanium was quantified by measuring the normalized
geometrical current density at potentials of 1.55 VRHE. The determined OER activity as a
function of layer thickness in Figure 49 a depicts a clear linear correlation. The influence of
layer thickness on ECSA is shown in Figure 49 b. Both, OER activity and ECSA show a
linear behaviour strongly suggesting that the complete film volume is available as the active
surface area contributes to the electrocatalytic oxygen evolution. In order to underline this
assumption, the OER activity is shown as a function of ECSA in Figure 49 c. The derived
OER activity at 1.55 VRHE scales linearly with the determined ECSA. Regardless of film
thickness each surface site thus contributes equally to the OER reaction, even for thicker
films and higher current densities. If any other process than the surface reaction such as gas
transport through the pore system, was the limiting step, a deviation from the linear behavior
would be expected for thicker films at least for higher potentials and current densities. As this
is not the case, transport limitations are absent in the case of iridium oxide catalyst films with
templated mesopores of at least up to 480 nm in thickness, at potentials of 1.55 VRHE and
current densities as high as 75 mA per cm2 of the planar electrode surface.
The Tafel plot is often used to investigate catalytic properties such as the i) rate determining
step of a postulated OER mechanism, ii) appearance of transport limitation of produced O2
gas, as well as iii) limited electron transport through catalytic layers. Figure 49 d show Tafel
plots for IrO2 with different layer thicknesses. The natural logarithm of the current density
from the respective 2nd iR corrected CV recorded in the OER potential window between 1.20
- 1.65 VRHE (Figure 25 c) has been used. However, only the corresponding current densities
at potentials higher than ca. 1.43 VRHE are shown (Figure 49 d), to only include potentials that
are causing currents attributed to the oxygen evolution reaction. The cyclic voltammograms
(Figure 25 c) and the derived Tafel plots (Figure 49 d) show a shift to lower overpotentials for
samples with higher layer thicknesses. The observed Tafel plots exhibit an almost linear
behaviour between E and log j at lower potentials (ca. 1.47 - 1.52 VRHE). However, higher
overpotentials strongly increase the Tafel slopes and produce “kinks” in the Tafel plot. In
order to investigate the potential and the current density at which the kink appears, a formal
criterion is defined: If the slope exceeds values greater than 1.1 times the Tafel slope, a kink
occurs (the first derivative of the Tafel plot was used for quantification, Figure A5 a)
Figure 49 e shows the determined kink potentials with respect to the layer thickness of IrO2.
The kinks occur independently of the layer thickness between 1.53 - 1.56 VRHE. It is unlikely
that the increase in Tafel slope is related to a limited electron transport through the layer
since IrO2 shows metallic conductivity. When considering the linear relationship between
OER activity and ECSA even at high current densities (75 mA/cm²), the increase in Tafel
slope can also not be due to the transport limitation of produced O2 within the pore system.
The determined corresponding current densities at the kinks underline this assumption, as
119
they appear to scatter around comparable low and high current densities (kink current
densities: 50 nm: 12.8 mA/cm²; 480 nm: 75.2 mA/cm²).
If the Tafel slope in the linear region is plotted as a function of layer thickness (Figure 49 f), it
attains a value of 52 - 55 mV/dec regardless of layer thickness and current density. If mass
transport limitation within the mesopore system is present, an increase in Tafel slope is
expected as the gas removal becomes the rate determining step. However, this is not the
case for IrO2 with different layer thicknesses at high current densities. The derived Tafel
slopes are in good agreement with reports in literature for thermally prepared iridium oxide:
40 - 60 mV/dec.[64, 126, 159] Moreover, it was reported that metallic iridium oxidized under acidic
OER conditions and exhibits similar Tafel slopes as thermally prepared iridium oxide: 40 -
60 mV/dec. [153, 160] Recently, Oezer et al.[137] published Tafel slopes for oxidized Ir(111)/(110)
single crystals. At lower potentials (1.52 - 1.58 VRHE) the Tafel slope amounts to 60 mV/dec
and 64 mV/dec for Ir(111) and Ir(110), respectively. However, sweeping to potentials higher
than 1.58 VRHE strongly increases the Tafel slope for both oxidized iridium single crystals
(Ir(111): 89 mV/dec, Ir(110): 83 mV/dec). The current densities measured at kinks are too
low (1 mA/cm²) for mass transport limitations.
In order to explain the increase in Tafel slopes at higher potentials McCrory et al.[38] has
stated the following: i) potential-dependent changes in the rate-determining step of the
catalytic mechanism, ii) repulsion of between adsorbed intermediates (which can be more
distinct at larger overpotentials due to a larger coverage of intermediates), and iii) blocking of
active sites by unreactive species.
These assumptions might be related, in the case of IrO2, to structural changes during OER.
Minguzzi et al.[161-162] reported, that IrIV slowly starts to transform to IrV at potentials around
1.30 VRHE. The transformation is accelerated with higher potentials, whereas a significant
amount of IrV is present at potentials around 1.50 VRHE. The transformation of IrIV to IrV at
higher potentials was further observed by the group of Nilsson.[163-164]
Based on the availability of data, we hypothesize that the transformation to higher oxidative
states of iridium at higher potentials leads to structural modifications which possibly affect the
rate determining step within the OER mechanism and strongly increases the Tafel slope.
In the current chapter (5.7) a linear relationship between OER activity and ECSA as a
function of layer thickness was established. Therefore, mass transport limitations were
excluded even at high layer thickness (480 nm) and high current density (75 mA/cm²). The
derived Tafel slopes were not only independent of the layer thickness and current densities,
with values as high as 52 - 55 mV/dec, but further excluded the presence of transport
limitations. However, applying high electrical potentials progressively increased the Tafel
slope possibly due to the transformation of IrIV to IrV, along with structural modifications
changing the rate determining step within the OER mechanism.
120
5.8 Tafel slope as a function of calcination temperature and potential
Changes in morphology and electrical conductivity as a function of calcination temperature
can now be related to electrochemical properties. Therefore, the Tafel plots of IrO2 and
IrO2/TiO2 were derived. Figure 50 presents the Tafel plots for different calcined samples
containing a) IrO2, b) IrO2/TiO2 (Ir(OAc)3+TiCl4) and c) IrO2/TiO2 (Ir(OAc)3+TALH). A further
evaluation of the Tafel plots reveal for all samples, the d) kink potentials and e) Tafel slopes
as a function of calcination temperature.
Figure 50: Tafel plots are presented for different calcined a) IrO2, b) IrO2/TiO2 produced from TiCl4
(30 wt. % Ir) and c) IrO2/TiO2 derived by TALH (30 wt. % Ir). For all investigated systems the observed d)
kink potentials and e) Tafel slopes with respect to the applied calcination temperature are shown. All
Tafel plots were derived from the upscan of the 2nd iR corrected CV (6 mV/s, 0.5 M H2SO4, 1600 rpm).
Figure 50 a shows that different heat treated IrO2 exhibit similar Tafel slopes in the range
between 50 - 54 mV/dec being in line with slopes reported for thermally prepared IrOx (40 -
60 mV/dec).[64, 126, 159] A steady increase of the Tafel slope is observed at higher potentials
producing kinks. The kinks were quantified (according to a procedure described in chapter
5.7) and show the following values: 1.55 VRHE (350 °C), 1.55 VRHE (375 °C), 1.54 VRHE
(400 °C), 1.54 VRHE (475 °C), 1.57 VRHE (550 °C), 1.59 VRHE (625 °C).
Figure 50 b depicts the Tafel plots of IrO2/TiO2 synthesized from Ir(OAc)3 and TiCl4 which
were thermally treated at different temperatures. The overpotential decreases with respect to
-1.5 -1.0-0.5 0.0 0.5 1.0 1.5 2.0 2.5
1.4
1.5
1.6
1.7
E vs. RHE / V
log j / mA cm
-2
geo
-1.5-1.0-0.5 0.0 0.5 1.0 1.5 2.0 2.5
1.4
1.5
1.6
1.7
E vs. RHE / V
log j / mA cm
-2
geo
-1.5-1.0-0.5 0.0 0.5 1.0 1.5 2.0 2.5
1.4
1.5
1.6
1.7
E vs. RHE / V
log j / mA cm
-2
geo
200 300 400 500 600
1.4
1.5
1.6
1.7
Kink potential E vs. RHE / V
T
calc
/ °C
200 300 400 500 600
0
50
100
150
200
250
Tafel slope / mV dec
-1
T
calc
/ °C
a) Tafel plots: IrO
2
(different T
calc.
)
350
375
400
475
550
625 °C
b) Tafel plots:
IrO
2
/TiO
2
(TiCl
4
)
c) Tafel plots:
IrO
2
/TiO
2
(TALH)
400 °C
500
600
400
500
600
200 °C 300
Ir(OAc)3
+ TiCl4IrO2
Ir(OAc)3
+ TALH
e) Tafel slopes vs. T
calc.
Ir(OAc)3
+ TiCl4IrO2
Ir(OAc)3
+ TALH
d) Kink potential vs. T
calc.
incomplete
template
removal
ongoing
sintering
high
surface
area
incomplete
template
removal
ongoing
sintering
high
surface
area
121
the calcination temperature between 200 to 400 °C. A further increase of calcination
temperature to values exceeding 500 °C reveals a progressive increase in overpotential. The
Tafel slope follows a very similar trend as observed for the overpotential. A steady decline is
noted for increasing temperatures of 200 °C (213 mV/dec) over 300 °C (98.5 mV/dec) to
400 °C (54.8 mV/dec). A successive increase is observed for higher calcination temperatures
such as 500 °C (58.6 mV/dec) and 600 °C (122 mV/dec). Moreover, only samples heat
treated at 300 °C (1.63 VRHE), 400 °C (1.55 VRHE) and 500 °C (1.58 VRHE) depict a kink
potential according to the previously defined criterion.
Figure 50 c shows Tafel plots for different heat treated IrO2/TiO2 (Ir(OAc)3 + TALH). Samples
calcined between 200 and 300 °C reveal Tafel slopes exceeding 2000 mV/dec. Therefore,
the respective samples are not considered in the discussion as the occuring current most
likely is not related to the oxygen evolution reaction. The lowest overpotential is observed for
samples heat treated at 400 °C and steadily increases when moving to higher temperatures:
400 °C (62 mV/dec), 500 °C (121 mV/dec) and 600 °C (155 mV/dec). However, only samples
calcined at 400 °C depict a kink potential as high as 1.57 VRHE.
In order to deduce global trends, Figure 50 d presents the observed kink potentials of all
systems with respect to the calcination temperature. The kink potentials of all systems occur
between 1.54 - 1.59 VRHE (Note: Ir(OAc)3+TiCl4 calcined at 300 °C still contains polymer
template and is not considered in the discussion). The respective kink potentials of IrO2 show
a slight increase as the calcination temperature is increased. A similar trend is observed for
IrO2/TiO2 derived by Ir(OAc)3 + TiCl4 as the kink potential increases from 400 to 500 °C. The
kink potential of Ir(OAc)3 + TALH calcined at 400 °C is found in similar regions such as for
similar calcined IrO2. The combined data of all systems reveal a slight increase in the kink
potential as a consequence of increasing calcination temperatures. The behaviour of the kink
potentials might be associated with the higher degree of crystallinity. If the kink is somehow
related to the transformation of IrIV to IrV,[161-164] possibly more crystalline materials are in
need of more energy (thus a higher potential) to undergo that transformation and cause a
strong increase in the Tafel slope. However, no other data were derived in order to underline
this theory. The observed kink potentials for IrO2 and IrO2/TiO2 as a function of applied
calcination temperature are reasonable in line with reports from literature for single crystals
of Ir(111) and Ir(110) (both ca. 1.58 VRHE).[137]
In Figure 50 e the Tafel slopes are plotted as a function of calcination temperature.
Interestingly, the Tafel slope of IrO2 seems to be independent of the applied calcination
temperature suggesting that structural modifications such as crystallinity are not sufficient
enough to change the rate determining step within the OER mechanism. Scheuermann et
al.[153] deposited different layer thicknesses of TiO2 by ALD on oxidized silicon substrates and
subsequently applied iridium as a catalyst onto TiO2 by PVD. The investigated
122
electrocatalytic performance in the OER regime as a function of TiO2 layer thickness
revealed an increase in Tafel slope for samples with a TiO2 layer thickness greater than
2 nm. The increase in Tafel slope is related to a hindered electron transport process through
the layer as a consequence of a lowered electrical conductivity. Therefore, we assume that
the constant slope of IrO2 as a function of calcination temperature indicates the absence of a
significant oxidation of the underlying titanium substrate. This behaviour is in line with reports
from the literature claiming that titanium covered by “thick” layers of IrO2 is shielded towards
oxidation.[57]
In the case of IrO2/TiO2 either produced from Ir(OAc)3 + TiCl4 or Ir(OAc)3 + TALH, the Tafel
slope remains high at calcination temperatures below 400 °C (Figure 50 e). In addition, the
ECSA (Figure 46 b), OER activity (Figure 46 a), and electrical conductivity (Figure 28 d,
Figure 34 d) of the corresponding samples appear low indicating incomplete template
removal. If the calcination temperature is increased to 400 °C, the polymer template seems
to be fully removed. Hence, an accessible pore system is observed with the capability to
provide a high OER activity (Figure 46 a). The observed Tafel slopes of such systems are
comparable to slopes determined for “pure” mesoporous templated IrO2. A further increase in
calcination temperature steadily increases the Tafel slope of IrO2/TiO2. For IrO2 it was found
that different calcination temperature, thus crystallinity does not significantly affect the Tafel
slopes (Figure 50 e). Under the assumption that this finding is valid for systems with mixed
metal oxides, the increase in Tafel slope is possibly related to the interaction between iridium
oxide and titanium oxide which form solid solutions at higher calcination temperatures
(Figure 28, Figure 34). This behaviour possibly changes the catalytic reactivity of iridium
centres in a way that an increase in the Tafel slope is the consequence.
123
5.9 Investigation of Tafel slopes as a function of iridium loading and potential
In order to evaluate the influence of iridium loading on the Tafel slopes, and kink potentials
Figure 51 shows Tafel plots of samples with different iridium loadings, such as IrO2/TiO2
produced by a) Ir(OAc)3 + TiCl4 and b) Ir(OAc)3 + TALH (Note: 100 wt. % Ir in Ir/TiO2
describes “pure, titanium free” IrO2). In addition, for all systems the observed c) kink
potentials and d) quantified Tafel slopes are shown.
Figure 51: The anodic scan of the 2nd iR corrected CVs are illustrated as Tafel plots for thermally prepared
(400 °C) a) IrO2/TiO2 from Ir(OAc)3 + TiCl4 and b) IrO2/TiO2 obtained with Ir(OAc)3 + TALH. Moreover, the
quantification of observed c) kink potentials and d) Tafel slopes are shown. (1.20 - 1.65 VRHE, iR corrected,
0.5 M H2SO4, 6 mV/s, 1600 rpm)
For IrO2/TiO2 (Ir(OAc)3 + TiCl4) Figure 51 a shows that the Tafel slopes drastically decrease
from 220 mV/dec (15 wt. % Ir in Ir/TiO2) to 58 mV/dec (30 wt. % Ir) and remain constant
against a further increase in iridium content: 60 mV/dec (60 wt. % Ir), 55 mV/dec (75 wt. %
Ir), 53 mV/dec (100 wt. % Ir equals to 50 nm IrO2). Moreover, a steady increase of the Tafel
slope with higher applied potentials is observed as a kink. The kinks occur at defined
potentials which were quantified according to a criterion introduced in chapter 5.7. The
observed kink potentials are as followed: 1.56 VRHE (30 wt. % Ir), 1.56 VRHE (60 wt. % Ir),
1.55 VRHE (75 wt. % Ir), 1.58 VRHE (100 wt. % Ir).
In analogy, Figure 51 b presents the Tafel plots of IrO2/TiO2 obtained from Ir(OAc)3 + TALH.
A similar trend is shown with the Tafel slope which strongly decreases from 211 mV/dec
(10 wt. % Ir in Ir/TiO2) over 112 mV/dec (15 wt. % Ir) to 63 mV/dec (30 wt. % Ir). A further
-1.5-1.0-0.5 0.0 0.5 1.0 1.5 2.0 2.5
1.4
1.5
1.6
1.7
E vs. RHE / V
log j / mA cm-2
geo
-1.5-1.0-0.5 0.0 0.5 1.0 1.5 2.0 2.5
1.4
1.5
1.6
1.7
E vs. RHE / V
log j / mA cm
-2
geo
020 40 60 80 100
1.4
1.5
1.6
1.7
Kink potential E vs. RHE / V
wt.% Ir in Ir/TiO2
020 40 60 80 100
0
50
100
150
200
250
Tafel slope / mV dec-1
wt. % Ir in Ir/TiO2
15 wt.% Ir 30 60 75
10 wt.% Ir 15 30 45 6075
Ir(OAc)3
+ TiCl4IrO2
Ir(OAc)3
+ TALH
Ir(OAc)3
+ TiCl4IrO2
Ir(OAc)3
+ TALH
a) Tafel plots:
IrO
2
/TiO
2
(TiCl
4
)
b) Tafel plots:
IrO
2
/TiO
2
(TALH)
d) Tafel slopes vs. T
calc.
c) Kink potential vs. T
calc.
100 100
124
increase in the iridium content reveals no significant influence on the Tafel slope: 62 mV/dec
(45 wt. % Ir), 52 mV/dec (60 wt. % Ir), 54 mV/dec (75 wt. % Ir) and 53 mV/dec (100 wt. % Ir).
The observed kinks in the Tafel plots were quantified (criterion from 5.7) and occur at the
following potentials: 1.54 VRHE (10 wt. % Ir in Ir/TiO2), 1.51 VRHE (15 wt. % Ir), 1.59 VRHE
(30 wt. % Ir), 1.58 VRHE (45 wt. % Ir), 1.56 VRHE (60 wt. % Ir), 1.56 VRHE (75 wt. % Ir) and
1.58 VRHE (100 wt. % Ir).
In order to deduce general trends Figure 51 c shows all observed kink potentials for
IrO2/TiO2, either derived by Ir(OAc)3 + TiCl4 or Ir(OAc)3 + TALH, as a function of iridium
loading. It is clearly visible that kink potentials for samples with loadings of 10 and 15 wt. % Ir
in Ir/TiO2 appear to be significantly lower than for higher loadings. As suggested by Figure
48, samples with low iridium loadings suffer from a hindered electron transport processes
through the layer which possibly affects the kink potential. However, if the iridium content
exceeds 30 wt. % Ir, the kink potentials are located in the same region as they are for
100 wt. % Ir (“pure” IrO2) and are related to changes in the rate determining step of the OER
mechanism affected by the transformation of IrIV to IrV.[38, 161-163]
Interestingly, the Tafel slopes depict a complementary behaviour (Figure 51 d) as they
steadily decrease with increasing iridium loadings from 10 to 30 wt. % Ir, but do not change
significantly with further increasing iridium. The higher Tafel slope for layers with low iridium
loadings is related to an insufficient degree of electrical conductivity as electrons travelling
through the layer away from the catalytic centre are delayed.[153] Moreover, the Tafel slope of
IrO2/TiO2 appears to be independent of morphological aspects as it is not changing with
different TiO2 precursors as long as a sufficient degree of conductivity is provided. Layers of
IrO2/TiO2 derived by Ir(OAc)3 + TiCl4 show largely segregated areas with ca. 100 nm in
diameter (Figure 43 p), whereas IrO2/TiO2 obtained with Ir(OAc)3 + TALH only depict small
segregated domains of IrO2 with ~2 nm (Figure 43 u), thus providing a more homogenous
morphology.
5.10 Deduced structure-activity relations
In the upcoming chapter all findings of this thesis are summarized in one scheme. It reflects
all investigated OER-controlling parameters (Figure 52 a), which were identified by a
controlled variation of different paramaters within the synthesis procedures (Figure 52 b), and
all electrocatalytic investigations (Figure 52, right column). The structure is affected by these
parameters leading to two possible conditions (Figure 52 c and d). By investigating the OER
activity of both conditions, structure-activity relations are deduced (Figure 52 e).
125
Figure 52: Different OER-controlling parameters were identified in the thesis (Figure 51 a). The OER-
controlling parameters are affected by parameters (Figure 51 b) varied during synthesis (Tcalc., Ir-loading,
withdrawal rate) or electrocatalytic testing (applied potential). The parameters affect the resulting
structure and lead to two possible conditions (Figure 51 c, Figure 51 d). The electrocatalytic performance
of both conditions was correlated in order to deduce structure-activity relations (Figure 51 e).
Calcination temperature highly affects crystallinity (Ir(OAc)3: Figure 24, Ir(OAc)3 + TiCl4:
Figure 28, Ir(OAc)3+TALH: Figure 34). The degree of crystallinity within a sample is either
characterized as low (XRD amorphous) or high (XRD reflections). An increase of calcination
temperature leads to enhanced crystallinity (Figure 24, Figure 28, Figure 34) and lowers the
ECSA (Figure 46 b). It was observed that samples with a low crystallinity exhibit a higher
overall OER activity than crystalline materials (Figure 46). However, a material with low
crystallinity is also characterized by a high ECSA. The observation in Figure 46 thus shows
the overlapping effects of crystallinity and ECSA on OER activity.
The electrical conductivity of layers coated on substrates is affected by two independent
synthesis parameters: the applied calcination temperature (IrOAc)3 + TiCl4: Figure 28,
Ir(OAc)3 + TALH: Figure 34) and the Ir loading (IrOAc)3 + TiCl4: Figure 31, Ir(OAc)3 + TALH:
Figure 37). A controlled variation of the calcination temperature simultaneously modified
crystallinity, electrical conductivity and accessible active surface area. Therefore, a variation
of the calcination temperature appears inappropriate in order to investigate the influence of
electrical conductivity on intrinsic reactivity separately. Therefore, the Ir content within TiO2
was varied, producing a lower intrinsic reactivity (Figure 48) as well as higher Tafel slopes
Electrical
conductivity
ECSA Layer thicknessCrystallinity
+
-
+
-
e
-
e
-
Deduced structure-activityrelations
low conductivity
high conductivity
low ECSA
high ECSA
low crystallinity
high crystallinity
low thickness
high thickness
low η
high η
low crystallinity
ispresent
high conductivity
ismeasured
large ECSA
isavailable
High OER
activityis
observed,
when:
layerthickness
ishigh. No sign
of transport
limitation
detected
OER-controlling
parameters
Condition1
Condition2
Parameters Tcalc. Tcalc., Ir loading Tcalc., Ir-loading
layerthickness
withdrawalrate
OER-potential
overpotential
islow (< 0.35 V)
potential
log j
E vs. RHE
~ 55 mV/dec
log j
E vs. RHE
> 70 mV/dec
b)
a)
c)
d)
e)
126
(Figure 51) for samples with loadings lower than 30 wt. % Ir in Ir/TiO2. Layers with Ir loadings
higher than 30 wt. % Ir in Ir/TiO2 exhibit the same intrinsic reactivity and Tafel slopes as for
“pure” mesoporous templated IrO2. The combined data suggest that a distinct electron
transport mechanism is present for samples with an insufficient electrical conductivity.
The active surface area is affected by the i) calcination temperature (Figure 46), ii) layer
thickness (Figure 49), and iii) iridium loading within TiO2 (Figure 48). All synthesis
parameters were varied and the resulting OER activities and active surface areas were
investigated. The combination of all obtained data suggests that if a sufficient degree of
conductivity is provided (> 30 wt. % Ir/TiO2, 0.1 S/m) the OER activity scales with the ECSA
suggesting that the ECSA must be one of the most relevant OER-controlling parameter.
The O2 evolution was investigated for layers consisting of mesoporous templated IrO2. The
ECSA and OER activity scaled linear with the layer thickness. In order to obtain samples with
different layer thicknesses, a controlled variation of the withdrawal rate during dipcoating was
carried out. If any other process than the surface reaction, such as gas transport through the
pore system, was the limiting step, a deviation from the linear behavior between OER activity
and ECSA would be expected. As this is not the case (Figure 49), the transport is not limited
in the case of iridium oxide catalyst films with templated mesopores of at least 480 nm in
thickness, at potentials of 1.55 VRHE and current densities of 75 mA/cm².
The influence of the OER-controlling parameters on observed Tafel slopes were investigated
for layers consisting of IrO2 and IrO2/TiO2. Within the investigated paramater range, the Tafel
slopes of IrO2 are unaffected by layer thickness (Figure 49), and calcination temperature
(Figure 50). The constant Tafel slopes as a function of layer thickness confirm the absence
of mass transport limitations. The steadiness of the slopes as a function of calcination
temperature can be related to the prevented oxidation from the underlying Ti substrate and
that crystallinity seems not to change the rate determining step in the OER kinetics.
The Tafel slope of mixed metal oxides such as IrO2/TiO2 shows very similar values as for
IrO2 with a loading of at least 30 wt. % Ir in Ir/TiO2 (Figure 51). The higher Tafel slope for
lower loadings is associated with a different electron transport mechanism most likely
induced by an insufficient degree of electrical conductivity. If the calcination temperature is
lower than 300 °C, the samples suffer from incomplete template removal thus causing a
higher Tafel slope as for samples calcined at 400 °C. Calcination at temperatures higher than
500 °C results in an increased Tafel slope and is related to crystallisation and the beginning
formation of solid solutions containing IrO2 and TiO2. The formation of a solid solution seems
to be unfavorable for the preparation of highly active OER electrocatalysts. At higher
potentials of ca. 1.55 - 1.60 VRHE, the Tafel plots exhibit an increased Tafel slope which is
related to a change in the rate determining step of the OER kinetics. We associate the
increase to the beginning transformation of IrIV to IrV.
127
5.11 Comparison of iridium-mass based OER activity
Chapter 5.11 presents a comparison of the iridium mass base related OER activity between
a) commercial catalysts and b) new mesoporous catalysts of this work. a) The reference
catalysts were deposited on titanium via an “ink”-procedure (chapter 4.5). The iridium mass
was determined by the volume drop-casted onto the substrate and the powder concentration
within the ink. b) IrO2 and IrO2/TiO2 with a high expected activity according to Figure 52 (low
crystallite size, sufficient electrical conductivity, high ECSA) were synthesized by dipcoating
a solution containing PEO-PB-PEO and different metal oxide precursors (e.g. Ir(OAc)3, TiCl4,
TALH) onto titanium sheets. The final catalysts were obtained by a subsequent heat
treatment at temperatures between 375 and 400 °C. In order to determine the OER activity
and the iridium mass before catalytic testing, each coated titanium sheet was blanked out
twice. For each catalytic system this technique provides two identical specimen with equal
geometrical iridium loading. The first specimen was dispersed in aqua regia and
subsequently treated in the micro wave to dissolve iridium oxide. The iridium mass was
finally quantified by ICP-OES. The second specimen and the commercial catalysts were
used as working electrodes.
Figure 53 shows SEM images of a) dropcasted inks of commercial catalysts onto titanium
cylinders and b) new mesoporous templated catalytic coatings of IrO2 and IrO2/TiO2. The
iridium mass based OER activity is included for the 50th and 100th CVs. On top of each
column the factors denote the relative iridium mass based OER activity of IrO2 powder,
IrO2/TiO2 (Ir(OAc)3+TiCl4), IrO2/TiO2 (Ir(OAc)3+TALH) and IrO2 (Ir(OAc)3) with respect to
commercial available IrOx/TiOx powder.
128
Figure 53: Investigation of morphology and iridium mass based OER activity for a) commercial catalysts
(IrOx/TiOx and IrO2 powder) and b) new catalysts with templated mesoporous structure (IrO2/TiO2
(Ir(OAc)3 + TiCl4), IrO2/TiO2 (Ir(OAc)3 + TALH) and IrO2 (Ir(OAc)3)). SEM images were obtained for inks
dropcasted on titanium cylinders and for mesoporous coatings on titanium sheets subsequent to heat
treatment at 400 °C and 375 °C, respectively. The morphology of commercial systems and mesoporous
catalytic coatings appear to be different in terms of porosity and homogeneity. The iridium mass before
catalytic testing was derived a) nominal and b) by ICP-OES. The OER activity was accessed by cyclic
voltammetric measurements in 0.5 M H2SO4 and 1600 rpm within a potential window of 1.20 - 1.65 VRHE
(6 mV/s). The current measured at 1.55 VRHE during the anodic scans of the 50th and 100th CVs were
normalized to the derived iridium mass. The factors on top of each column respresent the relative activity
with respect the reference system (ref.: IrOx/TiOx).
The stripes with brighter and darker appearance in the derived SEM images of dropcasted
inks for commercial IrOx/TiOx powders can be related to edge effects suggesting textural
roughness on the outer surface area (Figure 53 a). In contrast, IrO2 powders depict larger
areas with similar brightness. The absence of brightness variations is often related to a
smooth surface area appearing for materials with a higher degree of crystallinity. However,
IrOx/TiOx
(Elyst, Umicore)
no template
Nafion
183 µgIr cm-2
(nominally)
IrO2powder
(Sigma Aldrich)
no template
Nafion
13 µgIr cm-2
(nominally)
IrO2/TiO2
(Ir(OAc)3/TiCl4)
PEO-PB-PEO
30 wt. % Ir in Ir/TiO2
10min 400 °C
8.5 µgIr cm-2
(ICP)
IrO2/TiO2
(Ir(OAc)3/TALH)
PEO-PB-PEO
30 wt. % Ir in Ir/TiO2
10min 400 °C
4.3 µgIr cm-2
(ICP)
IrO2
(Ir(OAc)3)
PEO-PB-PEO
5 min 375 °C
42 µgIr cm-2
(ICP)
100 nm100 nm
SEM
b) New catalysts (this work)
100 nm
Sample
description
50th CV
400
300
200
100
500
OER mass activity
at 1.55 V vs. RHE / A g
Ir
a) Commercial catalysts
100th CV
500
400
300
200
100
OER mass activity
at 1.55 V vs. RHE / A g
Ir
x0.2
x24.4
x12.7
x26.3
x0.2
x17.4 x10.9
x23.9
ref.
ref.
100 nm 100 nm
-1
-1
129
PEO-PB-PEO templated samples clearly (Figure 53 b) reveal homogenous and crack free
layers with a film volume completely penetrated by mesopores.
During the 50th CV the iridium mass based OER activity of purchased IrO2 powder appears to
be 5 times smaller (x 0.2) than for IrOx/TiOx powder. In contrast, new mesoporous templated
catalysts from this work show a 24 (IrO2/TiO2: Ir(OAc)3+TiCl4), 13 (IrO2/TiO2: Ir(OAc)3+TALH)
and even 26 times (IrO2: Ir(OAc)3) higher iridium mass related OER activity. Similar relative
mass activities are observed for each system even after 100 CVs. The deduced structure-
activity relations can be used to explain the enhanced OER activity of new catalysts from this
work (see Figure 52). A high OER activity was observed for samples with i) a sufficient
degree of electrical conductivity, ii) a fast removal of produced O2 gas, iii) a low crystallinity
as well as iv) a high accessible active surface area.
The accessible surface area (ECSA) was determined by the mean value of the integrated
anodic and cathodic scans for CVs recorded within a potential window of 0.40 - 1.40 VRHE
(50 mV/s). The ECSA, iridium mass and ECSA normalized to the iridium mass is shown for
different catalytic systems in Table 3.
Table 3. ECSA and iridium normalized ECSA for commercial catalysts and new catalysts from this work.
Catalytic system ECSA / mC Ir mass / µg
ECSA per Ir mass
/ C g-1
Commercial: IrO
x
/TiO
x
(Umicore)
1.610
36
45
Commercial: IrO
2
(Sigma)
0.070
2.6
27
This work: IrO
2
/TiO
2
(Ir(OAc)3+TiCl4) 0.918 1.7 108
This work: IrO
2
/TiO
2
(Ir(OAc)3+TALH) 0.572 0.9 133
This work: IrO
2
(Ir(OAc)3) 3.560 8.3 660
All catalytic systems show different ECSA thus complicating the identification of a clear trend.
The difference in surface area is related to the different amount of iridium which is expected
to scale with the number of active sites. In order to correct the ECSA for the iridium mass, a
“specific surface area” is defined and expressed as ECSA per mass of iridium (C/gIr). It is
clearly visible that new catalytic systems of this work provide an at least 2 times higher
specific surface area. Our mesoporous templated coatings therefore further exploit the
performance of scarce iridium. The lower iridium mass related OER activity for commercial
systems can also be due the use of Nafion®. Nafion® is often added as a binder to attach the
catalyst on the surface of the substrate. However, reports in literature show a significant
decrease of electro catalytic performance when adding Nafion® as a binder.[165]
130
6 Conclusions and Outlook
The electrocatalytic splitting of water by using renewable energy sources such as wind and
solar power is regarded as a possible route for a sustainable energy economy. However, the
efficiency of water electrolyzer devices is limited by the complex reaction mechanism of the
oxygen evolution reaction (OER) resulting in a high anodic overpotential. The goal of this
work was the preparation of films with higher electrocatalytic oxygen evolution reaction
activity compared to commercial available catalyst powders and to understand structure-
activity relations. To achieve this goal a controlled variation of synthesis parameters during
the preparation of catalytic layers (i.e. NiO, IrO2 and IrO2/TiO2) was performed.
NiO films with an ordered mesopore structure were synthesized via soft-templating by
employing a metal complex formed from citric acid and nickel nitrate along with a polymer
template PEO213-PB184-PEO213. At calcination of 250 °C an amorphous carbonate is formed
which transforms into NiO at higher calcination temperature while retaining the templated
mesopore structure. All catalysts show a significant OER activity, whereby samples calcined
at 350 °C exhibit the highest OER performance and the highest surface area. A further
increase in OER activity for mesoporous NiO layers can be achieved by potentiostatic
treatments at 1.75 VRHE which is in line with reports in literature[27] and is explained by an in-
situ transformation from NiO to Ni(OH)2/NiOOH, with NiOOH being the active phase for OER.
Films of mesoporous IrO2 were obtained via a soft-templating approch based on micelles of
amphiphilic block copolymers PEO213-PB184-PEO213 and iridium acetate. The samples show
significant OER activity when calcined at temperatures higher than 350 °C. Heat treatment at
375 °C produces samples with ordered pores, low crystallinity, highest OER activity and
highest surface area. Thick mesoporous catalyst films were obtained by multilayer deposition
and show no signs of gas transport limitations even at current densities of 115 mA/cm2.
The synthesis of mixed metal oxides was performed by an amphiphilic triblock copolymer
PEO213-PB184-PEO213, iridium acetate and either TiCl4 or TALH. Different iridium loadings and
calcination temperatures between 200 - 600 °C were studied to convert deposited films into
mixed metal oxides of IrO2/TiO2 with tunable iridium loading and crystallinity. Samples of
IrO2/TiO2 obtained by iridium acetate and TiCl4 show largely segregated domains (ca.
100 nm) of IrO2 and TiO2 independently of the calcination temperature. Layers of IrO2/TiO2
produced by iridium acetate and TALH (400 °C), however, only show a small segregation of
ca. 2 nm. The highest OER activity and highest active surface area was observed for
samples calcined at 400 °C. The observed electrical conductivity significantly increases for
iridium loadings higher than 30 wt. % thus following percolation theory.
131
The investigation of structure-activity relationships revealed that the OER performance of
mesoporous IrO2 and IrO2/TiO2 is controlled by at least three independent factors, i.e. i) the
intrinsic reactivity per accessible site, ii) the electrical conductivity and iii) the accessible
surface area (ECSA).
i) At low calcination temperatures, the pore system is still partially blocked by the remaining
polymer template. High calcination temperatures decrease the ECSA due to sintering and
crystallite growth. Two different regimes of reactivity were identified for mesoporous IrO2. At
calcination between 350 and 475 °C iridium oxide with low crystallinity and high activity is
produced. However, at higher calcination temperatures a progressive crystallization and
decreasing OER activity is observed. Calcination at 375 °C thus produces the highest ECSA
and the highest reactivity. ii) The synthesis of mixed metal oxides of IrO2/TiO2 provided a
high ECSA and an optimal electron transport through the layer for samples with an iridium
content of at least 30 wt. % Ir in Ir/TiO2. At lower iridium content, the electrical conductivity is
insufficient thus causing an additional overpotential and a lowering of the intrinsic reactivity
per accessible active site. Higher iridium loadings successively increase electrical
conductivity as well as ECSA. However, the provided ECSA clearly depict a linear
relationship with the OER activity. Therefore we conclude that, if a sufficient degree of
electrical conductivity is achieved, the intrinsic reactivity of active iridium centres dispersed in
TiO2 is the same as for “pure” IrO2. iii) The produced monometallic Ir-oxide based OER
catalysts show the lowest overpotential reported so far in literature. Mesopores, introduced
into the catalyst by templating with micelles of block copolymers, allow a rapid transport of
the produced oxygen up to current densities of 75 mA/cm2. Thick mesoporous catalyst films
are obtained by multilayer deposition and did not show signs of gas transport limitations. The
catalyst films were mechanically stable even at current densities of 115 mA/cm2.
The developed films represent an example for homogeneous and scalable model systems to
investigate the influence of crystallinity, electrical conductivity and gas production rate on
intrinsic and overall OER activity. The films provide a narrow pore size distribution, a tunable
pore size, a controlled layer thickness and a high activity. The concept enables optimal use
of precious iridium. Moreover, the model system paves the way for quantitative investigations
of structure-activity relationships and transport properties in other gas evolution reactions.
Further work will extend the concept of highly conducting catalysts with a high active surface
area by focusing on more complex systems, e.g. niobium doped TiO2 with an additional
content of IrO2. Niobium is well known for its capabilities to enhance electron conductivity of
titanium oxide. By synergy of TiO2 and niobium sufficient conductivity is achieved even at low
iridium loadings, potentially leading to a higher iridium mass based OER activity.
132
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