Improvement of the kinetics of hydrogen release from ammonia borane confined in silica aerogel
Abstract
2018-09-20
Full text
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Imp o emen o he kine ics o hyd ogen elease om ammonia
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bo ane con ined in silica ae ogel
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Mi iam Rueda, Luis Miguel Sanz-Mo al, José Juan Sego ia, Ángel Ma ín*
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Depa men o Chemical Enginee ing and En i onmen al Technology - Uni e si y o
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Valladolid
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TERMOCAL Resea ch G oup – Uni e si y o Valladolid
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c/ Doc o Me gelina s/n 47011 Valladolid (Spain)
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Tel: +34 983423174, e-mail: [email p o ec ed] (Á. Ma ín)
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Imp o emen o he kine ics o hyd ogen elease om ammonia
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bo ane con ined in silica ae ogel
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Mi iam Rueda1, Luis Miguel Sanz-Mo al1, José Juan Sego ia2, Ángel Ma ín1*
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1Depa men o Chemical Enginee ing and En i onmen al Technology - Uni e si y o
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Valladolid, c/ Doc o Me gelina s/n 47011 Valladolid (Spain)
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2TERMOCAL Resea ch G oup – Uni e si y o Valladolid, c/ Paseo del Cauce 59 47011
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Valladolid (Spain)
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Tel: +34 983423174, e-mail: [email p o ec ed] (Á. Ma ín)
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Abs ac
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Ammonia bo ane is a p omising hyd ogen s o age ma e ial due o i s high g a ime ic
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capaci y (19.6 % w ), bu i also p esen s limi a ions such as a slow hyd ogen elease wi h
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a long induc ion ime, a di icul egene a ion, o he o ma ion o oams and gaseous by-
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p oduc s du ing he molysis. P e ious s udies ha e shown ha by nanocon inemen o
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ammonia bo ane wi hin a po ous suppo some o hese limi a ions can be o e come due
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o he educ ion and s abiliza ion o ammonia bo ane pa icle size. Howe e , his e ec
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was only obse ed wi h mode a e ammonia bo ane loadings, as wi h highe loadings he
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po es o he suppo became obs uc ed. In his wo k, silica ae ogels p oduced by CO2
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d ying, wi h po e olumes up o 2 cm3/g, ha e been used o con ine ammonia bo ane.
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The in luence o he amoun o ammonia bo ane loaded on he ae ogel suppo on he
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he mal and s uc u al p ope ies o he ma e ial has been analyzed. I has been ound ha
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mo e han 60 w % o ammonia bo ane can be e ec i ely s o ed in he po es o he
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ae ogel suppo . The esul ing ma e ial shows as e hyd ogen elease kine ics by
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he molysis a 80ºC, due o a signi ican educ ion in he mea size o ammonia bo ane
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a e con inemen and he pa icipa ion o SiOH and SiOSi g oups o silica ae ogel in he
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decomposi ion mechanism.
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Keywo ds: solid s a e hyd ogen s o age, ammonia bo ane, silica ae ogel,
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nanocon ined, supe c i ical ca bon dioxide.
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1. In oduc ion
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As ossil uel ese es a e inc easingly limi ed and hei use cons i u e a cons an sou ce
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o g eenhouse gases and o he en i onmen al p oblems, he de elopmen o al e na i e
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ene gy sou ces is a ac ing a conside able a en ion [1, 2]. In con as wi h ossil uels,
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which can be easily s o ed and used when needed, he p oduc ion o ene gy om mos
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enewable sou ces is a iable and i canno be di ec ly con olled. A possible solu ion
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o his limi a ion could be o use hyd ogen (H2) as an ene gy ec o , acco ding o he
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app oach commonly known as ‘hyd ogen economy’ o ‘hyd ogen socie y’ [3]:
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Hyd ogen can be p oduced om wa e (by elec olysis, he mal decomposi ion,
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he mochemical p ocesses, pho olysis e c.) using enewable ene gy sou ces, and s o ed
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un il needed. Fu he mo e, he e iciency o he combus ion o hyd ogen (by
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combus ion in in e nal combus ion engines, ca aly ic combus ion o uel cells) is high,
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and i is one o he mos en i onmen ally a o able uels, as i p oduces nea ly ze o
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gaseous emissions.
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A la ge scales, hyd ogen can be anspo ed h ough pipelines (gas H2) o anke s
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(liquid H2), and i is a good ene gy ec o wi h an ene gy densi y o 33 kwh/kg,
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con aining h ee imes mo e ene gy han any hyd oca bon uel on a weigh basis [4].
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Howe e , he s o age o hyd ogen in small mobile uni s such as ehicles o small
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elec onic equipmen is mo e challenging.
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These challenges can be quan i ied analyzing he a ge s se by he US Depa men o
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Ene gy o 2020 o au omo i e hyd ogen sys ems: a hyd ogen s o age g a ime ic
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capaci y o 5.5 w % and a olume ic capaci y o 0.040 kg/L, wi h a maximum cos o
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333$/kg H2 s o ed [5]. Hyd ogen s o age by some o mos ob ious sys ems using
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comp essed o condensed H2 canno ul ill hese equi emen s due o he physical
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p ope ies o hyd ogen. In he o me case, high p essu es (700 ba o each a olume ic
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concen a ion o 0.042 kg H2/L) o huge olumes a e needed, and in he la e , high
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ene gy consump ion is una oidable in o de o main ain he equi ed c yogenic
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empe a u es [6]. Fo hese easons, solid s a e hyd ogen s o age ma e ials ha e been
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in ensi ely s udied, as hyd a es [7], me al-o ganic amewo ks [8] o me allic and
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chemical hyd ides [9].
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Ammonia bo ane (AB) is conside ed as a p omising chemical hyd ide, due o i s high
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hyd ogen g a ime ic capaci y (19.6%w H2) and olume ic capaci y (140 g/L),
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mode a e decomposi ion empe a u e, non- oxici y [10] and s abili y a oom
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empe a u e, e en in he ange 50-60ºC, which is impo an om he poin o iew o
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sa e y and enginee ing implica ions [11]. The he mal decomposi ion o nea AB
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eleases one mole o hyd ogen pe mole o AB in each o he ollowing eac ions (1),
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(2) and (3) [12]. In he i s decomposi ion s ep, AB eleases H2 o ming a complex
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polyme ic aminobo ane (PAB) below i s mel ing poin (114 ºC):
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BH3NH3 → BH2NH2 + H2 T > 120ºC (1)
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The ea e , PAB decomposes abo e 120 ºC, o ming polyme ic iminobo ane and small
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ac ions o undesi able ola ile byp oduc s:
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BH2NH2 → 1/3 (BHNH)3 + H2 T > 120ºC (2)
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(BHNH) → BN + H2 T > 500ºC (3)
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Ne e heless, he use o his compound as hyd ogen s o age ma e ial also aces some
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impo an limi a ions. One o hem is he kine ic limi a ion due o he long induc ion
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ime needed o dis up he dihyd ogen bonding and ini ia e he elease o hyd ogen.
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Fu he mo e, AB is di icul o egene a e: a e he molysis, i is no possible o es o e
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he ini ial AB by di ec hyd ogena ion, and complex chemical egene a ion ou es
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comp ising se e al s eps a e needed. Addi ionally, i o ms oams du ing he molysis
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ha also complica e he egene a ion due o he dis up ion o he physical s uc u e o
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he ma e ial. Mo eo e , du ing he decomposi ion p ocess, he emission o some ola ile
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byp oduc s as bo azine, dibo ane o ammonia can be eleased which could be poisonous
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o downs eam p ocesses and, pa icula ly, hyd ogen uel cells.
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Se e al s a egies ha e been es ed o o e come hese ba ie s, including he addi ion o
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ca alys s as silicon (Si), nickel (Ni), u henium (Ru), palladium (Pd) o zinc (Zn) [13-
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16], con inemen o ammonia bo ane in o po ous solid suppo s [17-21], dissolu ion o
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AB in ionic liquids [22,23] o using polyme s composi es [24]. Rega ding con inemen
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o AB, di e en suppo s ha e been es ed: silica sca olds as SBA-15 o MCM-48 [18],
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me al o ganic amewo ks (MOF) [16, 25] o ca bon based ma e ials [17] among o he s.
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The amoun o AB ha has been success ully loaded in he suppo depends on hei
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s uc u al p ope ies (SBET and Vpo es), ge ing a maximum amoun o 50%w using silica
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sca olds [17]. In all he cases ha ha e been epo ed, hyd ogen kine ic and
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he modynamic p ope ies ha e been imp o ed espec o nea hyd ide due o he
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educ ion in mean size. In ou p e ious wo k [26], mic opa icles o silica ae ogel we e
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used as suppo , ge ing a maximum concen a ion o 5%w AB loaded in hyd ophobic
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silica ae ogel. Liquid an isol en echnique was used o p ecipi a e he hyd ide p io
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supe c i ical ca bon dioxide d ying, esul ing in enhanced hyd ogen elease kine ic
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compa ed o pu e AB.
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In his wo k, we epo he con inemen o AB using silica ae ogel as po ous hos . The
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ae ogel has been p oduced by liquid o supe c i ical CO2 d ying, a echnique ha
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enables o p oduce a silica ma e ial wi h a high po e olume, and a co espondingly
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high po en ial capaci y o s o age o ammonia bo ane inside i s po es. Se e al samples
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wi h di e en concen a ions o AB up o 60 w % ha e been p epa ed in o de o
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analyze he in luence o he loading o AB on he he mal and s uc u al p ope ies o
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he ma e ial. Scanning elec on mic oscopy, N2 adso p ion iso he ms, FT-IR
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spec oscopy and X- ay di ac ion ha e been used in o de o cha ac e ize he inal
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p oduc p io o he measu emen o hyd ogen elease kine ics by decomposi ion a
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80ºC.
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2. Expe imen al me hods
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2.1 Ma e ials
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Te ame hylo hosilica e (TMOS, 98.0% pu i y), ammonium hyd oxide (NH4OH, 28.0-
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30.0% ammonia pu i y) and ammonia bo ane (AB, 97% pu i y) we e supplied by
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Sigma-Ald ich. Figu e 1 shows a mic og aph o nea AB as ecei ed. As shown in his
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Figu e, AB was cons i u ed by agglome a ed pa icles wi h sizes in he ange o 100 m
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and wi h a po ous s uc u e. Me hanol (MeOH; 99.8% pu i y), n-hexane (95% pu i y)
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and d y e ahyd o u an (THF; wi h maximum wa e o 0.0075w %) we e pu chased
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om Pan eac. Ca bon dioxide (CO2, 99.95% pu i y) was supplied by Ca bu os
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Me álicos S.A.
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(FIGURE 1)
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2.2 P epa a ion o AB loaded in silica ae ogel mic opa icles
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As p esen ed in Figu e 2, he p ocedu e o he p epa a ion o AB-loaded silica ae ogel
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mic opa icles consis s o h ee key s eps: p epa a ion o silica gel mic opa icles,
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addi ion o ammonia bo ane by a we imp egna ion me hod, and d ying o he AB-
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loaded gel pa icles wi h p essu ized ca bon dioxide in o de o p oduce he inal, d y
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AB-loaded ae ogel mic opa icles.
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(FIGURE 2)
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In he i s s ep o his p ocedu e, hyd ophilic silica alcogel was p epa ed using he well-
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known me hod o hyd olysis condensa ion sol-gel eac ion, using TMOS as p ecu so
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and me hanol as sol en . While wi h his p ocedu e i is common o p epa e la ge gel
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monoli hs, in his wo k he gel was syn he ized as mic opa icles, in o de o educe he
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possible hea and mass ans e esis ances ha could be caused by la ge ae ogel
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monoli hs. To do his, and acco ding o he p ocedu e desc ibed in a p e ious wo k [26],
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he sol-gel eac ion media was dispe sed in hexane unde mechanical s i ing, in o de o
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ob ain small d ople s o TMOS in me hanol dispe sed wi hin he hexane con inuous
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phase. A e 10 minu es o mechanical s i ing o his mix u e wi h a wo bladed axial
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s i e se a 600 pm, an aqueous solu ion o NH4OH was added as condensa ion
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ca alys , which induced he gela ion o TMOS. The mola a io used was he ollowing:
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1 mol TMOS: 4.4 mol MeOH: 3.3 mol H2O: 4.5 mol hexane: 0.08 mol NH4OH. As
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me hanol o wa e p oduced du ing he condensa ion eac ion can induce he
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decomposi ion o ammonia bo ane du ing he subsequen d ying p ocesses [26], a e 2
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hou s o gela ion he alcogel mic opa icles we e e ie ed and imme sed in THF. Gel
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pa icles we e hen kep du ing 7 days imme sed in THF in a closed essel, o le he gel
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age and s eng hen i s s uc u e. Du ing his ageing pe iod, he THF sol en was
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enewed a leas wice in o de o emo e he las aces o me hanol and wa e .
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A e he ageing p ocess, mic opa icles o alcogel a e eady o we imp egna ion,
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adding a solu ion o ammonia bo ane dissol ed in THF. This me hod has he ad an age
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ha imp egna ion can be pe o med unde milde empe a u e condi ions compa ed o
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mel in il a ion, and only one imp egna ion s ep is necessa y in con as o incipien
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imp egna ion me hods [27]. Again, THF was used ins ead o me hanol as sol en in
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o de o a oid me hanolysis and he e o e he decomposi ion p ocess o he hyd ide no
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only du ing we imp egna ion (due o SiOH g oups) bu also du ing d ying p ocess [26].
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Di e en samples wi h di e en concen a ions o ammonia bo ane we e p epa ed,
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adding di e en amoun s o hyd ide (0-0.4g AB dissol ed in 5mL o THF) o 2 g o
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mic opa icles o alcogel (gel be o e d ying, he e o e wi h he po es illed wi h he
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o ganic sol en ) in o de o s udy his in luence on he p ope ies o he inal solid
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p oduc . Wi h his, concen a ions o AB in he inal p oduc anging om 10 o 60 w %
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AB we e ob ained, whe e he concen a ion o AB is de ined as p esen ed in equa ion
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(4):
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(4)
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The hi d and las s ep is he emo al o he o ganic sol en in o de o ob ain he inal,
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d y AB/SiO2 pa icles. The d ying me hod employed is a key aspec ha de e mines he
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ex u al p ope ies o he po ous suppo . I he sol en is emo ed by e apo a ion o
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lyophiliza ion, he capilla y s esses associa ed o he o ma ion o apo -liquid
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in e aces inside he po es o he suppo cause ac u es and a pa ial collapse o he
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po e s uc u e o he ma e ial. In he case o SiO2 ma ixes, he ma e ials ob ained by
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hese d ying me hods usually show po e olumes below 0.5 – 1.0 cm3/g. Some
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examples a e he well-known SBA-15 o MCM-41 mesopo ous silica ma ixes. In
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con as , i p essu ized o supe c i ical ca bon dioxide is used o ex ac he sol en , he
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collapse o he po e s uc u e is minimized, because unde hese condi ions ca bon
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dioxide can be comple ely miscible wi h he o ganic sol en , and he e o e he
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ex ac ion p oceeds wi hou o ma ion o gas-liquid in e aces and wi hou capilla y
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s esses. Due o his enhanced p ese a ion o he po e s uc u e, wi h his me hod i is
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possible o each po e olumes in he ange 2 – 4 cm3/g [28]. Addi ionally, du ing his
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d ying p ocess CO2 can ac as an isol en o solu es dissol ed in he o ganic sol en , as
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i is comple ely miscible wi h he o ganic sol en , bu i canno dissol e high-molecula
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weigh solu es dissol ed in he o ganic sol en . This p ecipi a ion me hod is commonly
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e e ed in he li e a u e as “Gas An i Sol en ” (GAS) o “Supe c i ical An i Sol en ”
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(SAS) p ecipi a ion [29,30]. In he case o his wo k, as ammonia bo ane is insoluble in
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CO2 [26], when he THF-imme sed alcogels a e mixed wi h CO2, AB dissol ed in he
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THF ha ills he po es o he alcogels quickly p ecipi a es acco ding o a GAS
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p ecipi a ion mechanism, hus a o ing he o ma ion o small pa icles wi hin he po es
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o he gels.
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In a p e ious wo k, i was obse ed ha due he in e ac ion o AB wi h he SiO2 ma ix,
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he empe a u e needed o ini ia e he decomposi ion o AB is d as ically dec eased [26].
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Thus, in o de o a oid he he molysis o AB, he d ying p ocess was ca ied ou a a
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nea -ambien empe a u e o 25ºC and a a p essu e o 100 ba , hus employing
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p essu ized, liquid CO2. As in he p e ious wo k [26], a ba ch d ying appa a us,
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depic ed in Figu e 2, was used. Using his appa a us, he alcogels imme sed in THF
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we e loaded in o he ex ac ion essel and he sys em was p essu ized wi h CO2 using an
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ai -d i en pis on pump. The sys em was slowly p essu ized a a a e o 0.5 ba /min in
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o de o a oid b eakages in he alcogel/ae ogel and mechanical s esses ha could
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damage he s uc u al p ope ies o he inal p oduc . Once he desi ed p essu e and
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empe a u e we e eached, he eci cula ion pump ha connec s he ex ac ion essel
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wi h he CO2 ese oi was connec ed, hus bubbling CO2 h ough he THF-imme sed
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alcogels and enhancing he ex ac ion o he sol en . As CO2 g adually becomes
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sa u a ed wi h he sol en du ing he ex ac ion p ocess, CO2 in he sys em was enewed
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he mapping o samples wi h highe concen a ion o AB, up o he maximum
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concen a ion o 60 w % es ed in his wo k.
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(FIGURE 5)
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3.2.2 XRD pa e ns
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Figu e 6 shows he XRD pa e n o nea ammonia bo ane, which ma ches well wi h
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JCPDS e e ence 01-074-0894 sugges ing he ypical polyc ys alline s uc u e wi h
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e agonal la ice symme y, in ag eemen wi h li e a u e in o ma ion abou he s uc u e
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o AB a ambien empe a u e [42]. The c ys alli e size es ima ed using he Sche e ’s
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equa ion o mula is 40 nm, and he dominan sha p peak o he pa e n is loca ed a
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23.75º, co esponding o (110) planes. A e ec ys alliza ion by GAS p ocess, sligh
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modi ica ions in he XRD pa e n can be obse ed a 2 = 17 and 30º. A simila
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modi ica ion can be obse ed in silica-loaded AB samples, al hough wi h less de ined
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peaks due o he s ong signal p oduced by he silica suppo . This modi ica ion in he
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pa e n can sugges he o ma ion o diammonia e o dibo ane (DADB), an isome o
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AB. This compound shows some di e ences ega ding he hyd ogen elease mechanism
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compa ed o i s isome AB: he empe a u e o decomposi ion o DADB is abou 10ºC
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lowe han ha o AB, and DADB unde goes solid-phase decomposi ion wi hou
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mel ing o induc ion pe iod e en a mode a e empe a u e, while AB su e s om a long
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induc ion pe iod p io o H2 elease [43]. The e o e, he o ma ion o his compound
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may jus i y some o he obse ed he mal p ope ies, as i will be discussed in he
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ollowing sec ions.
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Ne e heless, in GAS ec ys allized samples, he dominan pa e n is equi alen o ha
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o nea AB, also co esponding o e agonal c ys al s uc u e is obse ed, al hough
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di ac ion peaks a e no so well de ined, and he es ima ed c ys alli e size inc eases o
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75 – 150 nm. In he case o AB loaded in silica ae ogel, he peaks a e me ged, he e o e
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sugges ing a educ ion o c ys allini y o an inc eased inhomogenei y in he p ope ies
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o he c ys als due o he inco po a ion in he po es [44]. Addi ionally, as shown in
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Figu e 5b i can be seen ha he XRD pa e n o amo phous silica, cha ac e ized by a
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b oad peak a ound 24º, is o e laid o he dominan peaks ela ed o AB. The e o e
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esul s show ha AB e ains i s c ys alline s uc u e a e nanocon ina ion wi hin he
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po es o he ae ogel, wi h es ima ed c ys alli e sizes in he ange 100 – 200 nm, simila
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o hose ob ained by ec ys alliza ion o AB by GAS p ocess.
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(FIGURE 6)
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3.3 The mal cha ac e iza ion o AB-loaded silica ae ogels
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Figu e 7 shows he di e en ial scanning calo ime y (DSC) aces o nea and
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ec ys allized AB compa ed o samples in which he hyd ide is loaded in silica ae ogel.
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In he case o he cu e o nea AB, a sha p endo he mic peak is obse ed whose onse
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empe a u e (Ton=108.5 ºC) and peak empe a u e (Tp=110.8ºC) is d ama ically educed
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when AB is loaded in silica ae ogel (see able 2). This i s peak is associa ed o he
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mel ing poin [14] o he dissocia ion o he in e molecula hyd ogen bonding [18]. The
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educ ion o elimina ion in his i s peak sugges s ha he deg ee o hyd ogen bond in
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he samples in which AB is embedded in silica ae ogel is dec eased, a o ing he
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educ ion o he induc ion ime. A simila esul has been obse ed when AB was
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embedded in o he silica suppo s [18]. Rega ding ec ys allized AB, DSC esul s also
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show educ ion in he onse and peak endo he mic empe a u es, main aining he shape
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o he cu e o nea AB. In his case, a ia ions in cha ac e is ic empe a u es o he
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DSC aces can be associa ed o he educ ion in he mean pa icle size achie ed by
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ec ys alliza ion o AB. As desc ibed by Va in e al [45], a educ ion o pa icle size
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in o he subic ome ic o nanome ic scale is gene ally associa ed o a educ ion o he
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onse and peak empe a u es o hyd ogen e olu ion he mal e en s, due o he
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des abiliza ion o he ma e ial induced by he inc eased pa icle su ace. Addi ionally,
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he educ ion o onse empe a u es and induc ion ime can be associa ed o he
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o ma ion o DADB by ec ys alliza ion sugges ed by XRD assays.
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Simila esul s ha e been ob ained in o he wo ks whe e AB is con ined in di e en
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suppo s. In he case o SBA and MCM silica suppo s, educ ions in he onse and peak
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empe a u es o 48ºC and 100ºC ha e been epo ed [18], bu as p e iously desc ibed
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lowe empe a u es ha e been ob ained in his wo k. This ac can be due o he highe
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olume o po es o ae ogel suppo ha a oids he agglome a ion o AB in meso-
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channels. The e o e highe con ac be ween he pa icle and he su ace o he silica
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ae ogel akes place, enhancing he in luence o silica su ace g oups on he
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decomposi ion mechanism. In expe imen s wi h MOFs [42] o ca bon c yogels [17, 20]
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as suppo s, simila modi ica ions in he he mal esponse o he ma e ial ha e been
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epo ed. Howe e , S ini as e al. [16] obse ed a educ ion o 30ºC in he onse and
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peak empe a u es o decomposi ion using MOFs, whe eas in ou case a displacemen o
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almos 70ºC is ob ained.
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Mo eo e , DSC esul s indica e a educ ion o he exo he mic en halpy associa ed wi h
424
hyd ogen elease as he p opo ion silica/AB is inc eased. The measu ed en halpy o
425
eac ion o H2 elease om nea AB is -24.9 kJ/mol AB, which is in good ag eemen
426
wi h esul s epo ed in li e a u e. Howe e , when he p opo ion silica/AB is inc eased,
427
he co esponding en halpy o eac ion changes o -10.9 kJ/mol AB o he sample wi h
428
60% o AB, and -5.5 kJ/mol AB o he sample wi h 30% o AB. A educ ion o he
429
en halpy o eac ion o H2 elease om AB was also obse ed by Gu owska e al. [40]
430
in hei s udies o inco po a ion o AB in mesopo ous SBA-15 silica sca old. Howe e ,
431
hese au ho s epo a mo e d as ic a ia ion o he en halpy o -1.0 kJ/mol AB. These
432
19
au ho s indica e ha he eason o he educed exo he mici y is he supp ession o he
433
o ma ion o bo on compounds as byp oduc s o he PAB ha is he main
434
decomposi ion p oduc o AB acco ding o eac ion 1, which had he a o able
435
consequence o educing he p oduc ion o gaseous byp oduc s.
436
(TABLE 2)
437
(FIGURE 7)
438
This hypo hesis ag ees well wi h he esul s ob ained in his wo k by TGA assays.
439
Figu e 8 shows he esul s o TGA analysis pe o med on nea AB and AB-loaded silica
440
ae ogel. In he case o nea AB, wo impo an weigh loss s eps, which co espond o
441
he decomposi ion o he hyd ide, a e obse ed: he i s one ill 129ºC co esponds o a
442
weigh loss o 12.7 w % and he second one, which inishes a 213ºC, co esponds o a
443
weigh loss o 27.5 w %. In compa ison, and in ag eemen wi h he esul s o DSC
444
assays, TGA analysis shows ha he AB con ined in silica ae ogel ini ia es i s
445
decomposi ion a lowe empe a u es. I is also no iceable ha in his case, weigh loss
446
is no con ined o sha p s eps a de ined empe a u es, bu i p oceeds con inuously o e
447
he empe a u e ange s udied. In pa icula , a empe a u es abo e 200ºC, whe e as
448
p e iously discussed nea AB does no expe ience any addi ional weigh losses, a
449
con inuous weigh loss is s ill obse ed in he case o AB con ined in ae ogel. This
450
esul indica es ha he hi d s ep o he he mal decomposi ion mechanism, indica ed in
451
eac ion (3), also begins a lowe empe a u es in he case o con ined AB compa ed o
452
nea AB. Mo eo e , as shown in Table 2, in bo h cases he o al weigh loss pe uni
453
mass o AB in he sample is signi ican ly la ge han he maximum amoun o hyd ogen
454
ha can s o ed in he compound. Simila esul s ha e been epo ed in [18], sugges ing
455
ha when AB is hea ed o high empe a u es abo e 200ºC, o he gases apa om
456
hyd ogen a e p oduced, as bo azine, dibo ane, ammonia, e c. Howe e , analyzing he
457
20
esul s epo ed in Table 2, i is no iceable ha he o al amoun o ola ile compounds
458
p oduced by hea ing up o 300ºC is educed when AB is con ined in silica ae ogel. This
459
esul , oge he wi h he a ia ions in DSC assays o con ined AB p esen ed be o e,
460
sugges ha in e ac ions be ween AB and he silica suppo a e aking place ha
461
in luence he decomposi ion mechanism o AB. Such in e ac ions we e sugges ed o
462
happen be ween AB and hyd oxyl g oups om he silica su ace o he hos by Lai e al.
463
[18]. These g oups can in e ac wi h he BH3 g oup, loosening he co alen bond
464
be ween BH3 and NH3 g oups o AB, hus des abilizing and p omo ing he
465
decomposi ion o he compound. Fu he mo e, by his in e ac ion BH3 is kep bound o
466
he sca old educing he p oduc ion o bo azine and p ecluding he o ma ion o
467
poliiminobo ane
468
(FIGURE 8)
469
In igu e 9, FTIR o nea AB and AB loaded in silica ae ogel is shown be o e and a e
470
dehyd ogena ion a 80ºC. I is obse ed ha mos o he peaks a equencies ela ed o
471
N-H and B-H bonds a e b oadened, shi ed and dec eased o in ensi y which indica es
472
he dis up ion o he bonds due o he elease o hyd ogen [13] in bo h samples. The
473
same beha io is obse ed o all he concen a ions o AB loaded in silica ae ogel,
474
al hough i is mo e p onounced a highe concen a ions o AB. B-N band in he ange
475
700-900 cm-1, which is obse ed in all he samples, is weakened bu is s ill de ec ed
476
a e dehyd ogena ion; his ac cla i ies ha B-N is no dis up ed and ammonia
477
o ma ion is a oided du ing he decomposi ion [14]. On he o he hand, in he sample in
478
which AB is loaded, he bonds ela ed o silica a e p esen wi hou any change a e
479
he mal ea men due o i s s abili y a hese condi ions.
480
(FIGURE 9)
481
21
Rega ding he c ys allini y o he samples a e he mal dehyd ogena ion, igu e 10
482
shows XRD analyses o byp oduc a e iso he mal dehyd ogena ion a 80ºC. Acco ding
483
o ICDD 00-019-0418, 2θ= 20.1º, 23.6º and 41.1º a e assigned o amo phous PAB
484
(NH2BH2)5 [46]. In he case o AB/SiO2 samples, amo phous silica peak is p esen apa
485
om amo phous PAB byp oduc .
486
(FIGURE 10)
487
3.4 Kine ics o hyd ogen elease by he molysis a 80ºC
488
Figu e 11 shows he kine ics o hyd ogen elease by he molysis a 80ºC o nea AB
489
compa ed wi h AB con inemen in silica ae ogel. Resul s in his igu e a e no malized
490
epo ing he amoun o hyd ogen eleased by uni mass o AB in he sample. Due o he
491
design o he cell used o measu e kine ics, i was no possible o analyze samples o he
492
gas e ol ed du ing hemolysis. Howe e , i is assumed ha a his empe a u e, he gas
493
which is eleased is H2 [12, 19, 41, 47] and no o he ola ile gases a e p esen in he gas
494
s eam in nea AB no con ined in silica ae ogel. Rega ding he shape o he cu e in
495
nea AB, i ollows a sigmoidal kine ic, ypical o nuclea ion and g ow h pa hway, wi h
496
a long induc ion ime o mo e han 2 h, as epo ed in p e ious wo ks [48]. A e
497
con inemen in silica, he induc ion ime is educed signi ican ly. This means ha he
498
silica could ac as a ca alys (SiOH g oups) [40] c ea ing de ec si es in he suppo ha
499
ini ia e he decomposi ion a lowe empe a u e. On he o he hand, a lowe
500
concen a ion o AB in he solu ion (p io o he d ying), he hyd ide could p ecipi a e in
501
he po es o he silica wi h lowe mean size as was also sugges ed wi h XRD analyses
502
and co obo a ed in BET esul s. This sugges s ha smalle pa icles ha e mo e con ac
503
wi h he su ace o he silica and an easie way o o m di e en bonds be ween he wo
504
ee pai o elec ons o O in he Lewis base o Si-O-Si o Si-OH bond om he silica
505
22
wi h BH3 o NH3 om AB. As esul , he in e molecula hyd ogen bond is educed,
506
ollowing he mechanism p oposed by Lai e al. [18].
507
In he case o nea AB, 2 hou s a e needed o s a eleasing H2, and mo e han 4 hou s
508
o ge hal o i s con en in H2 a his empe a u e (0.025gH2/gAB) whe eas only i akes
509
22 minu es in he case o 13%AB loaded in silica ae ogel. This ac shows he
510
imp o emen o silica ae ogel as suppo o his chemical hyd ide sys em.
511
Rega ding o ec ys allized sample, i can be obse ed ha he elease p o ile main ains
512
he sigmoidal shape cha ac e is ic o nea AB, wi h a slowe hyd ogen elease han
513
samples loaded in silica ae ogel du ing he i s 30 min o he molysis. Howe e ,
514
compa ed wi h nea AB, wi h he pa icle size educ ion achie ed by GAS
515
ec ys alliza ion he induc ion ime is d as ically educed and he elease o hyd ogen is
516
accele a ed, o he poin ha a e one hou an equi alen amoun o hyd ogen is
517
eleased om GAS- ec ys allized AB as om AB loaded silica ae ogel wi h a 30 w %
518
o AB.
519
(FIGURE 11)
520
As a complemen o Figu e 11, Table 3 p esen s he o al hyd ogen elease pe uni mass
521
o solid p oduc (AB + silica ae ogel suppo ). Resul s in his able clea ly indica e he
522
weigh penal y caused by he use o silica ae ogel as po ous hos , as his ma e ial does
523
no con ibu e o he hyd ogen s o age capaci y, hus educing he o al g a ime ic
524
capaci y o he ma e ial [27]. Howe e , i can be seen ha his disad an age is
525
coun e balanced by a as e hyd ogen elease du ing he i s 1-2 h o he molysis.
526
(TABLE 3)
527
Mo eo e , he e is a signi ican isual change in he mo phology o nea AB in con as
528
o AB encapsula ed in silica ae ogel. Figu e 12 shows he di e en esul o AB a e
529
23
he mal decomposi ion a 80ºC. In he case o nea AB, oaming p ocess akes place a
530
he same ime ha H2 is eleased om he hyd ide. Thus, e en i he ma e ial was
531
mic onized be o e he molysis, his mo phology and i s associa ed ad an ages a e
532
comple ely los du ing he he molysis and he e o e in possible u u e hyd ogen cycles,
533
i he ma e ial is egene a ed [49]. Howe e , when AB is encapsula ed in silica ae ogel,
534
his p ocess is a oided ob aining pa icles wi h he same physical appea ance. To
535
con i m his obse a ion, Figu e 13 p esen s SEM/EDX mic og aphs o he
536
60%AB/SiO2 sample a e he molysis. As shown in his igu e, he o iginal
537
mo phology o he ma e ial is p ese ed a e he he molysis. Fu he mo e, as indica ed
538
by he esul s o ni ogen mapping, he decomposi ion p oduc s o AB emain
539
homogeneously dispe sed wi hin he SiO2 ae ogel ma ix. The e o e i can be concluded
540
ha by inco po a ion o AB inside he ae ogel he mo phological a ia ions o he
541
ma e ial due o oaming a e a oided.
542
(FIGURE 12)
543
(FIGURE 13)
544
4. Conclusions
545
Ammonia Bo ane has been ec ys allized and nanocon ined inside he po es o silica
546
ae ogel by a no el p ocess, based on a simul aneous ae ogel d ying and ammonia
547
bo ane gas an isol en p ecipi a ion using comp essed ca bon dioxide. Due o he
548
a o able ex u al p ope ies o he ae ogel ma e ials ob ained wi h his me hod, i has
549
been possible o load ae ogels wi h up o 60 w % o ammonia bo ane, wi hou blocking
550
o po es and wi h a homogeneous dispe sion o ammonia bo ane wi hin he ae ogel. By
551
analysis o he he molysis p ocess, i has been obse ed ha by nanocon inemen he
552
empe a u e equi ed o ini ia e he he molysis p ocess is educed and he elease
553
kine ics a e accele a ed as hey do no show induc ion ime. Fu he mo e, by
554
24
nanocon ina ion o AB, he mo phological p ope ies o he ma e ial a e s abilized and
555
oaming is elimina ed, which could be a o able p ope ies o a subsequen ma e ial
556
egene a ion p ocess. The easibili y o implemen a ion o he mul i-s ep chemical
557
p ocess equi ed o e-hyd ogena e AB when his compound is embedded in he silica
558
ma ix emains o be es ed.
559
560
Supplemen a y In o ma ion
561
Video 1: The molysis o nea ammonia bo ane a 80ºC. Time is accele a ed by a ac o
562
o 64.
563
Video 2: The molysis o 60%AB/SiO2 sample a 80ºC. Time is accele a ed by a ac o
564
o 64.
565
566
Acknowledgemen s
567
This esea ch has been inanced by he Spanish Minis y o Economy and
568
Compe i i eness h ough p ojec ENE2011-24547. Á. Ma ín hanks he Spanish
569
Minis y o Economy and Compe i i eness o a Ramón y Cajal esea ch ellowship. M.
570
Rueda hanks he Uni e si y o Valladolid o a FPI p edoc o al g an . L. M. Sanz
571
hanks he Spanish Minis y o Economy and Compe i i eness o a FPI p edoc o al
572
g an .
573
Re e ences
574
[1] M.Bala , In . J. Hyd ogen Ene g. 33 (2008) 4013-4029
575
[2] M.Hook, X.Tang, Ene g. Policy 52 (2013) 797-809
576
[3] S. A. She i , F. Ba bi , T. N. Vezi oglu, Elec ici y J. 18 (2005) 62-76
577
[4] J. G ae z, Chem. Soc. Re . 38 (2009) 73-82
578
25
[5] DOE: US Depa men o Ene gy. Web si e: h p://www.doe.go .
579
[6] L. O. Williams, D. E. Spond, Appl. Ene g. 6 (1980) 99-112.
580
[7] H. P. Veluswamy, R. Kuma , P. Linga, Appl. Ene g.122 (2014) 112-132.
581
[8] M. Paik Suh, H. J. Pa k, T. K. P asad, D. Lim, Chem. Re . 112 (2012) 782-835
582
[9] B.Sakin una, F.Lama i-Da k im, M.Hi sche , In . J. Hyd ogen Ene g. 32 (2007)
583
1121-1140
584
[10] B. Peng, J. Chen, Ene g. En i on. Sci. 1 (2008) 479-483
585
[11] S. D. Rassa , C. L. Aa dahl, T. Au ey, R. S. Smi h, Ene g. Fuel. 24 (2010) 2596-
586
2606
587
[12] G. Wol , J. Baumann, F. Bai alow, F. P. Ho mann, The mochim. Ac a 343 (2000)
588
19-25
589
[13] D. Kuma , H. A. Mangal edeka , S. K. Mahajan, Ma e . Renew. Sus ain. Ene gy 3
590
(2014) 23
591
[14] A. C. Gangal, P. Kale, R. Edla, J. Manna, P. Sha ma, In . J. Hyd ogen Ene g. 37
592
(2012) 6741-6748
593
[15] B. Roy, J. Manna, P. Sha ma, J. Alloy Compd. 645 (2015) S234-S238.
594
[16] G. S ini as, J. Fo d, W. Zhou, T. Yildi im, In . J. Hyd ogen Ene g. 37 (2012)
595
3633-3638
596
[17] A. Fea e , S. Sepeh i, P. Shambe ge , A. S owe, T. Au ey, G. Cao, J. Phys. Chem.
597
B 111, (2007) 7469-7472
598
[18] S-W Lai, H-L. Lin, T.L.Yu, L-P. Lee, B-J. Weng, In . J. Hyd ogen Ene g. 37
599
(2012) 14393-14404
600
[19] T.Au ey, A.Gu owska, L.Li, J.Linehan, M.Gu owski, P ep in s o Pape s-
601
Ame ican Chemical Socie y, Di ision o Fuel Chemis y 49 (2004) 150-151
602
[20] S.Sepeh i, B.B.Ga cia, G.Cao, J. Ma e . Chem. 18 (2008) 4034-
603
32
Table 2. - Tempe a u e da a and weigh losses o nea and ec ys allized AB s loaded
699
in silica ae ogel wi h di e en concen a ion ob ained om DSC and TGA analyses
700
espec i ely.
701
702
Sample
Ton1
(ºC)
Tp1
(ºC)
Ton2
(ºC)
Tp2
(ºC)
To al w
loss pe
w AB
Nea AB
108.5
110.8
113.9
114.1
40.2
Rec ys allized AB
70.5
77.9
102.4
113.4
-
60% AB/SiO2
37.6
62.3
84.8
108.9
33.0
30% AB/SiO2
39.5
68.7
83.1
99.0
-
33
Table 3. - Amoun o H2 eleased a di e en imes by iso he mal he molysis a 80ºC in
703
nea and ec ys allized s. AB loaded in silica ae ogel wi h di e en concen a ion
704
15min
30min
45min
1h
2h
inal
Sample
mgH2/g o al
mgH2/g o al
mgH2/g o al
mgH2/g o al
mgH2/g o al
mgH2/g o al
nea AB
0
0
0
0
2
52
AB ec ys allized
1,66
7,45
20,19
30,45
43,98
52
13%AB/SiO2
2,26
4,28
5,28
5,80
6,38
6,76
30%AB/SiO2
1,69
4,43
7,30
9,07
12,31
14,56
60%AB/SiO2
2,48
9,42
17,79
20,65
27,27
32,24
705
34
Figu es
706
707
708
Figu e 1. - SEM mic og aph o nea ammonia bo ane as ecei ed
709
710
35
1. Syn hesis alcogel
3. L-CO2 d ying
(100ba /25ºC)
2. Addi ion o AB
solu ion
PI
TI
co2
PI
Liquid en
Reci cula ion
pump
CO2
bu e
Ex ac o
CO2 pump
Ho ai o en
711
Figu e 2. - S eps o p epa a ion o silica ae ogel mic opa icles loaded wi h ammonia
712
bo ane.
713
714
36
715
Figu e 3. FTIR spec a o a) silica ae ogel b) nea AB c) ec ys allized AB
716
d)30%AB/SiO2 e)60%AB/SiO2. Cu es a e e ically displaced o cla i y.
717
718
37
719
Figu e 4.-Ni ogen adso p ion-deso p ion iso he ms and BJH po e size dis ibu ion o
720
silica ae ogel and AB loaded in silica wi h di e en concen a ion ( ) adso p ion ( )
721
deso p ion
722
723
38
724
Figu e 5.- SEM images o A) Rec ys allized AB a e ec ys alliza ion in THF using
725
liquid CO2 as d ying me hod B) 30%AB loaded in silica ae ogel and mapping o sample
726
B (blue is e e ed o silica and ed o Ni ogen)
727
728
39
729
Figu e 6. –a) XRD o nea ammonia bo ane, ec ys allized ammonia bo ane and AB
730
loaded in silica ae ogel wi h di e en concen a ions b) Ampli ica ion o XRD signal
731
showing he cha ac e is ic pa e n o silica ae ogel. Cu es a e e ically displaced o
732
cla i y
733
734
40
735
Figu e 7. - DSC cu es o AB and AB loaded in silica ae ogel wi h di e en
736
concen a ion. The cu es a e no malized acco ding o he weigh o AB, and e ically
737
displaced o cla i y.
738
739
41
740
Figu e 8. - TGA cu es o AB and AB loaded in silica ae ogel
741
742