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Effect of magnetite transformations on degradation efficiency of cerium dioxide-magnetite composite

Abstract

Present investigations are focused on synthesis of magnetite/cerium dioxide reactive sorbents in various weight ratios of components and their characterization of chemical and magnetic properties. The morphology and changes in magnetic transformations in dependence on composition are followed by electron microscopy, X-ray diffraction, Mossbauer spectroscopy and magnetic measurements at room and low temperatures. Degradation efficiency is evaluated from a decomposition of the organophosphorus pesticide parathion methyl using prepared reactive sorbents. The experimental results reveal that the degradation efficiency, expressed by rate constant (mol/h) in dependence on amount of cerium dioxide content (vol.%), is independent on kind of iron oxide but increases with cerium dioxide content. On the contrary, saturation and remanent magnetizations are highly sensitive to relative ratio of iron oxides; magnetite, maghemite and hematite, originating from the initial magnetite transformations in dependence on sample composition.

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Effect of magnetite transformations on degradation efficiency of cerium dioxide-magnetite composite

Author: Jirásková, Yvonna
Publisher: Elsevier
Year: 2020
DOI: 10.1016/j.jmrt.2020.02.068
Source: https://dspace.vsb.cz/bitstreams/e5137a2b-ce67-4cea-a3cc-d6b5ae5089cb/download
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www.jm .com.b
A ailable
online
a
www.sciencedi ec .com
O iginal
a icle
E ec
o
magne i e
ans o ma ions
on
deg ada ion
e ficiency
o
ce ium
dioxide-magne i e
composi e
Y onna
Ji asko aa,∗,
Ji i
Bu sika,
Jakub
Ede e b,
Pa el
Janosb,
Jan
Ju icac,
Ji i
Lunacekd,
Ond ej
Zi o skyd
aCEITEC
IPM,
Ins i u e
o
Physics
o
Ma e ials,
AS
CR, ˇ
Ziˇ
zko a
22,
616
62
B no,
Czech
Republic
bFacul y
o
he
En i onmen ,
Uni e si y
o
Jan
E angelis a
Pu kynˇ
e,
K álo a
V´
yˇ
sina
7,
400
96
Ús í
nad
Labem,
Czech
Republic
cRegional
Ma e ials
Science
and
Technology
Cen e,
Vˇ
SB
–
Technical
Uni e si y
o
Os a a,
17.
Lis opadu
2172/15,
708
00
Os a a-Po uba,
Czech
Republic
dDepa men
o
Physics,
Vˇ
SB
–
Technical
Uni e si y
o
Os a a,
17.
Lis opadu
2172/15,
708
00
Os a a-Po uba,
Czech
Republic
a
i
c
l
e
i
n
o
A icle
his o y:
Recei ed
26
Decembe
2019
Accep ed
18
Feb ua y
2020
A ailable
online
28
Feb ua y
2020
Keywo ds:
CeO2
I on
oxide
Mic os uc u e
Magne ic
p ope y
Mössbaue
spec oscopy
Deg ada ion
e ficiency
a
b
s
a
c
P esen
in es iga ions
a e
ocused
on
syn hesis
o
magne i e/ce ium
dioxide
eac i e
so -
ben s
in
a ious
weigh
a ios
o
componen s
and
hei
cha ac e iza ion
o
chemical
and
magne ic
p ope ies.
The
mo phology
and
changes
in
magne ic
ans o ma ions
in
depen-
dence
on
composi ion
a e
ollowed
by
elec on
mic oscopy,
X- ay
di ac ion,
Mössbaue
spec oscopy
and
magne ic
measu emen s
a
oom
and
low
empe a u es.
Deg ada ion
e ficiency
is
e alua ed
om
a
decomposi ion
o
he
o ganophospho us
pes icide
pa a hion
me hyl
using
p epa ed
eac i e
so ben s.
The
expe imen al
esul s
e eal
ha
he
deg a-
da ion
e ficiency,
exp essed
by
a e
cons an
(mol/h)
in
dependence
on
amoun
o
ce ium
dioxide
con en
( ol.%),
is
independen
on
kind
o
i on
oxide
bu
inc eases
wi h
ce ium
diox-
ide
con en .
On
he
con a y,
sa u a ion
and
emanen
magne iza ions
a e
highly
sensi i e
o
ela i e
a io
o
i on
oxides;
magne i e,
maghemi e
and
hema i e,
o igina ing
om
he
ini ial
magne i e
ans o ma ions
in
dependence
on
sample
composi ion.
©
2020
The
Au ho s.
Published
by
Else ie
B.V.
This
is
an
open
access
a icle
unde
he
CC
BY-NC-ND
license
(h p://c ea i ecommons.o g/licenses/by-nc-nd/4.0/).
1.
In oduc ion
The
a e
ea h
ce ium
oxide
o
ce ium
dioxide
belongs
p esen ly
o
equen ly
s udied
opic.
I
is
p epa ed
by
a ious
syn he ic
p ocedu es
and
cha ac e ized
wi h
la ge
numbe
o
expe imen al
me hods.
Among
echnologies,
e.g.,
sol-gel
me hods,
homogeneous
hyd olysis
[1],
hyd o he mal
syn he-
∗Co esponding
au ho .
E-mail:
[email p o ec ed]
(Y.
Ji asko a).
sis
[2,3],
p ecipi a ion
me hods
using
oxala e,
ammonium
hyd oxide
and
ammonium
ca bona e
[4–6]
can
be
men ioned.
Ce ium
dioxide
and
ce ium
dioxide-based
composi es
a e
used
in
di e en
echnological
applica ions
[7].
These
include
a
wide
ange
o
ca aly ic
applica ions
[8],
solid
oxide
uel
cells
[9,10],
oxygen
senso s
[11],
glass-polishing
[12],
an
ul a io-
le
abso ben ,
e.g.,
o
cosme ic
use
[13,14],
eac i e
so ben s
[15–17].
The
las
decade
assumes
also
impo ance
in
he
medical
field.
Thanks
o
ce ium
dioxide
sel
egene a ing
an ioxidan
p ope ies,
i
ep esen s
a
p omising
an ioxidan
o
healing
nume ous
un ea able
oxida i e-s ess- ela ed
diseases
[18–21].
h ps://doi.o g/10.1016/j.jm .2020.02.068
2238-7854/©
2020
The
Au ho s.
Published
by
Else ie
B.V.
This
is
an
open
access
a icle
unde
he
CC
BY-NC-ND
license
(h p://
c ea i ecommons.o g/licenses/by-nc-nd/4.0/).
4432
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Ce ium
dioxide
is
he
mos
widely
known
compound
o
ce ium.
I
c ys allizes
in
fluo i e
c ys al
s uc u e
wi h
cc
uni
cell,
space
g oup
Fm3m.
I
has
pale
yellow
colou
and
is
p ac ically
insoluble
in
wa e
and
only
mode a ely
soluble
in
s ong
mine al
acids.
I
can
abso b
small
amoun
mois u e
and
ca bon
dioxide
om
he
a mosphe e.
The
p ope y
ha
is
equen ly
discussed
a
p esen
is
i s
easy
o ma ion
o
oxy-
gen
acancies
which
should
be
a
eason
o
i s
e omagne ic
beha iou
in
he
nanosized
s a e
(pa icle
dimensions
<
15
nm)
[22,23]
in
spi e
o
i s
diamagne ic
s a e
in
he
bulk
o m.
Ge
and
co-au ho s
[24]
e ified
expe imen ally
and
heo e ically
ha
oxygen
acancies
cause
an
inc ease
in
magne iza ion
o
nanopa icles
compa ed
o
bulk
samples
due
o
e ec -
ing
he
su ounding
o
elec ons
leading
o
an
inc ease
in
magne ic
momen s
o
pa icles.
The
oom- empe a u e
e -
omagne ism
o
ce ium
dioxide
is
also
influenced
by
ei he
goal-di ec ed
ansi ion
me al
doping
[25–28]
o
by
magne ic
impu i ies
[29,30].
P e ious
s udies
e ealed
an
unusual
abili y
o
ce ium
oxide
o
des oy
oxic
o ganophospha e
compounds;
his
abil-
i y
demons a es
no
only
in
pu e
nano-ce ium
dioxide,
bu
also
in
magne ically
sepa able
composi es
based
on
Fe-oxides
and
CeO2.
Va ious
chemical
p ocedu es
we e
examined
and
sui able
composi ions
and
he mal
ea men s
a e
sea ched
and
s udied
[15,31,32].
P esen
wo k
is
also
de o ed
o
magne ically
sepa able
so -
ben s
based
on
i on
and
ce ium
oxides
o
di e en
mu ual
olume
a ios
and
exposed
o
he
same
calcina ion
ea -
men .
The
mic os uc u al
and
physical
cha ac e is ics
o
hese
sys ems
ha e
been
s udied
in
o de
o
co ela e
hem
wi h
he
sensing
p ope ies
owa ds
haza dous
o ganophos-
pha es.
2.
Expe imen al
2.1.
Ma e ials
and
sample
p epa a ion
The
inpu
ma e ials
o
he
sample
p epa a ions
we e
pu -
chased
as
eagen -g ade
chemicals
om
Sigma
Ald ich
(S einheim,
Ge many).
The
ce ium
ca bona e
was
p epa ed
om
he
comme cial
Ce(NO3)3.6H2O
(pu i y
99.9%)
and
NH4HCO3(pu i y
99.5%)
by
p ecipi a ion
me hod
published
elsewhe e
[15].
B iefly,
he
ca bona e
p ecu so
was
p e-
pa ed
by
p ecipi a ion
o
an
aqueous
solu ion
o
Ce(NO3)3
(0.2
mol
L−1)
wi h
an
excess
o
NH4HCO3(0.5
mol
L−1)
unde
s i ing.
A e
he
p ecipi a ion
p ocess,
he
agi a ion
con in-
ued
o
one
mo e
hou
and
he
p ecipi a e
was
le
in
he
solu ion
un il
he
nex
day.
The
p ecipi a e
was
sepa a ed
by
fil a ion,
washed
wi h
deionized
wa e
and
d ied
o e nigh
a
110 ◦C.
Subsequen ly
he
adequa e
mass
o
ce ium
ca bon-
a e
and
a ificial
magne i e
(Fe3O4pa icle
size
50–100
nm)
was
mechanically
mixed
in
a ios
om
0/100
up
o
50/50
(CeO2/Fe3O4).
The
mix u es
o
ce ium
ca bona e/Fe3O4we e
subjec ed
o
annealing
p ocess
a
500 ◦C
o
2
h
in
ai
a mo-
sphe e.
Du ing
annealing
ce ium
ca bona e
ans o ms
in o
ce ium
oxide
(CeO2).
2.2.
Scanning
and
ansmission
elec on
mic oscopy,
X- ay
di ac ion,
pa icle
size
analyze
The
mo phology
o
samples
we e
ollowed
by
TESCAN
LYRA
3XMU
FEG/SEM
scanning
elec on
mic oscope
a
accele a ing
ol age
o
20
kV,
equipped
wi h
an
X-Max80
Ox o d
Ins u-
men s
de ec o
o
ene gy-dispe si e
X- ay
(EDX)
analysis.
FEI
Ti an
Themis
60–300
cubed
high
esolu ion
ansmission
elec-
on
mic oscope
wi h
a
high
sensi i i y
EDX
sys em
(0.7
s ad
solid
angle)
ope a ing
a
300
kV
was
used
o
selec ed
samples
o
see
hei
mo phology
in
mo e
de ails.
X’PERT
PRO
di ac ome e
(Panaly ical)
equiped
wi h
Co
K␣
adia ion
(␭
=0.17902
nm)
was
used
o
di ac og am
measu e-
men s
in
he
ange
o
2
=
20◦–135◦,
s eps
=
0.01◦,
and
ime/s ep
5
s.
Rie eld
s uc u e
efinemen
me hod
[33]
using
he
High-
Sco e
Plus
p og am
and
he
ICSD
da abase
[34]
we e
applied
o
analyze
he
ela i e
abundance
o
phases
(A)
and
hei
basic
pa ame e s,
la ice
cons an
(a)
and
mean
mic o-domain
size
(d).
Pa icle-size
dis ibu ion
was
measu ed
by
lase
di ac ion
pa icle
size
analyze
Mas e Size
3000,
Mal e n
Ins umen s
L d.
2.3.
Magne ic
and
Mössbaue
measu emen s
Room
empe a u e
magne ic
measu emen s
in
an
applied
ex e nal
field
o
±1600
kA/m
(±2
T)
we e
pe o med
using
ib a ing
sample
magne ome e
(VSM)
EZ9
(Mic osense,
Massachuse s,
USA).
This
equipmen
was
used
also
o
measu emen s
o
he
ini ial
( i gin)
cu e,
MVIR(H),
and
magne iza ions
a
inc easing
(MUP)
and
dec easing
(MDOWN)
posi i e
magne ic
fields.
These
cha ac e is-
ics
a e
needed
o
de e mina ion
o
he
Henkel
plo :
M(H)
=
MVIR(H)
−
(MUP(H)
+
MDOWN(H))/2.
A
physical
p ope y
measu emen
sys em
(PPMS,
Model
P935A,
San
Diego,
USA)
quan um
design
was
applied
o
mea-
su emen s
o
hys e esis
loops
wi h
maximal
magne ic
field
o
±4000
kA/m
(±5
T)
and
ze o-field-cooled
(ZFC)
and
field-
cooled
(FC)
cu es
in
he
magne ic
field
o
8
kA/m
and
in
he
empe a u e
ange
(2–293
K).
Mössbaue
spec oscopy
(MS)
measu emen s
we e
done
in
ansmission
geome y
a
oom
empe a u e
using
a57Co
(Rh)
sou ce.
Calib a ion
o
he
eloci y
scale
was
pe o med
wi h
␣-Fe
a
RT
and
he
isome
shi s
a e
gi en
wi h
espec
o
i s
Mössbaue
spec um.
All
spec a
we e
e alua ed
using
he
ansmission
in eg al
app oach
in
he
p og am
CONFIT
[35].
The
expe imen al
poin s
we e
analysed
by
double-
and
single-line
componen s
yielding
alues
o
isome
shi
(ı)
and
quad upole
spli ing
().
The
ela i e
ep esen a ion
o
hese
subcomponen s
is
deno ed
by
A.
2.4.
Deg ada ion
e ficiency
Deg ada ion
e ficiency
was
de e mined
om
pa a hion
me hyl
(PM)
decomposi ion
in o
4-ni o enol
(FN);
see
Re .
[15]
o
mo e
de ails.
The
simple
eac ion
PM⇒FN
is
assumed
and
kine ics
o
such
eac ion
is
ollowed
ei he
on
a
weigh
loss
j
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4433
Fig.
1
–
Sample
o
nominal
composi ion
Fe3O4+10
w .%
Ce2(CO3)3a e
calcina ion
ea men ;
le
panel
–
a ea
EDX
analyses
om
he
sp ead
powde ,
igh
panel
–
local
analyses
om
indi idual
cons i uen s.
The
ob ained
composi ions
(in
a .%)
a e
shown
below.
Fig.
2
–
Mo phology
as
seen
in
SEM,
seconda y
elec ons
(a)
and
XRD
di ac og am
(b)
o
magne i e
in
he
ini ial
s uc u al
s a e.
o
PM
o
an
inc ease
o
FN
amoun .
Unde
p esump ion
ha
no
o he
eac ion
exis s
he
loss
o
PM
should
be
equal
o
he
inc ease
o
FN.
This
was
alid
in
p esen
s udy.
3.
Resul s
and
discussion
3.1.
Mo phology,
phase
and
chemical
composi ion
Chemical
analysis
was
done
by
EDX
in
SEM
on
powde s
sp ead
on
a
conduc i e
ape.
Se e al
a eas
we e
selec ed
a
each
sam-
ple
and
he
in eg al
alues
we e
measu ed.
Along
wi h
la ge
a ea
analyses,
he
poin
EDX
analyses
o
indi idual
phases
we e
measu ed
as
well.
As
an
example,
he
sample
o
nom-
inal
composi ion
Fe3O4+10
w .%
Ce2(CO3)3a e
calcina ion
ea men
(500 ◦C/2
h/ai )
is
shown
in
Fig.
1.
To
ollow
changes
in
phase
composi ion
o
he
mixed
samples
a e
calcina ion
ea men ,
bo h
inpu
powde s,
i.e.
magne i e
and
ce ium
ca bona e,
we e
also
ea ed
sepa a ely
by
he
same
calcina ion
pa ame e s.
The
mo phology
o
ini ial
magne i e
is
seen
in
Fig.
2a
and
X- ay
di ac og am
anal-
ysed
using
ICSD
20596
da a
shee
is
depic ed
in
Fig.
2b.
The
4434
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Fig.
3
–
Mo phology
as
seen
in
SEM,
seconda y
elec ons
(a)
and
XRD
di ac og am
(b)
o
magne i e
a e
calcina ion
ea men
a
500 ◦C/2
h/ai .
calcina ion
ea men
a
500 ◦C
o
2
h
in
ai
did
no
b ing
any
isible
changes
in
mo phology
as
seen
in
Fig.
3a.
Ne -
e heless
he
XRD
measu emen
(Fig.
3b)
yielded
a
mix u e
o
h ee
Fe-oxides,
namely
hema i e,
␣-Fe2O3, maghemi e,
␥-
Fe2O3,
and
ini ial
magne i e
Fe3O4analysed
using
da a
shee s
15840,
35643,
and
20596,
espec i ely.
The
calcina ion
ea men
has
ans o med
ce ium
ca bon-
a e
in o
ce ium
dioxide
o med
by
hin
ela i ely
la ge
pla es
seen
in
Fig.
4a
simul aneously
wi h
i s
di ac og am
in
Fig.
4b
confi ming
pu e
ce ium
oxide
analysed
by
28753
ICSD
da a
shee .
The
ela i e
a ios
o
oxide
phases
measu ed
by
XRD
a e
summa ised
in
dependence
on
he
ini ial
nominal
sam-
ple
composi ion
in
Table
1.
The
esul s
show
p edominan ly
magne i e
ans o ma ion
du ing
calcina ion
ea men .
EDX
elemen al
mapping
in
TEM
was
used
o
wo
selec ed
samples
(S5
and
S9)
o
isualize
quali a i ely
elemen s
dis-
ibu ion.
In
bo h
samples
(Fig.
5a,b)
we
could
obse e
la ge
Ce- ich
oxides
and
fine
Fe- ich
oxides
wi h
almos
no
chem-
ical
in e mixing
and
wi h
mo phology
simila
o
he
ini ial
s a e.
The
same
image
was
ound
in
o he
mixed
samples:
he
mo phology
and
lay-ou
was
simila
o
ha
seen
in
Fig.
1
igh .
The
pa icle
size
dis ibu ion
is
depic ed
in
Fig.
6.
The
sam-
ple
wi h
he
lowes
ce ium
dioxide
con en
(S4)
ollows
he
dis ibu ion
o
Fe-oxide
pa icles.
A
highe
ce ium
dioxide
con en s
he
peaks
o
dis ibu ions
ollow
ei he
peaks
co -
esponding
o
Fe-
and
Ce-oxides
o
he
isible
b oadening
o
dis ibu ions
a e
p esen
eflec ing
pa icle
agglome a ions.
The
analysis
o
XRD
pa e ns
has
yielded
he
size
o
mic odomains
o
ce ium
dioxide
a ying
be ween
8
and
10
nm,
while
hose
o
Fe-oxide
phases
was
app oxima ely
en
imes
la ge .
The
la ice
pa ame e s
o
indi idual
phases
in
he
sam-
ples
sligh ly
fluc ua ed
wi hin
he
ange
o
expe imen al
e o .
No
sys ema ic
elonga ion
o
con ac ion
o
la ice
pa ame e s
indica e
subs i u ion
o
Fe3+(Fe2+)
in
CeO2o
Ce4+ in
Fe-oxide
phases.
The
samples
S5
and
S7
ha e
shown
highe
con en s
o
magne i e
and
maghemi e
bu
a
eason
o
i
is
a
p esen
unclea .
3.2.
Mac o-
and
mic omagne ic
p ope ies
The
magne ic
measu emen s
a
oom
empe a u e
we e
used
o
de e mina ion
o
basic
magne ic
pa ame e s,
sa u a ion
and
emanen
magne iza ions
and
coe ci i y
and
pa ame-
e s
needed
o
Henkel
plo s
[36].
Hys e esis
loops
including
de ail
a
low
magne ic
fields
a e
shown
in
Fig.
7
o
ini ial
magne i e
(S1),
magne i e
a e
calcina ions’
ea men
(S2)
in
he
le
panel
and
hose
o
ce ium
dioxide
(S3)
in
he
igh
panel.
The
cu e
o
ce ium
dioxide
consis s
o
e omag-
ne ic
con ibu ion
well
isible
in
de ail
and
he
diamagne ic
con ibu ion
eflec ed
by
dec easing
magne isa ion
a
highe
magne ic
fields
due
o
a
nega i e
magne ic
suscep ibili y.
A
dec ease
in
sa u a ion
magne iza ion
o
he
S2
sample
is
due
o
ans o ma ion
o
magne i e
in o
mainly
haema i e
con-
ibu ing
wi h
i s
low
alue
o
sa u a ion
magne iza ion.
The
hys e esis
loops
o
he
mixed
samples
a e
p esen ed
he e
by
means
o
hei
magne ic
cha ac e is ics
shown
in
dependence
on
sample
composi ion
in
Fig.
8.
A
low
sp ead
o
he
coe ci i y
alues
in
he
samples
co -
esponds
o
he
simila
mo phology
o
he
samples
seen
in
SEM
mic og aphs.
On
he
o he
hand,
he
non-mono onic
changes
in
sa u a ion
and
emanen
magne iza ions
ollow
changes
in
he
Fe-oxide
ep esen a ion.
The
highe
ela i e
ep esen a ion
o
magne i e
and
maghemi e
s.
haema i e
in
he
samples
S5
and
S7
(Fig.
8
uppe
panel)
ma kedly
influence
he
magne iza ion.
While
haema i e
is
weakly
e omagne ic
o
sa u a ion
magne iza ion
0.3
Am2/kg
a
oom
empe a u e,
he
magne i e
and
maghemi e
a e
e imagne ic
yielding
isi-
bly
highe
alues
o
sa u a ion
magne iza ion
anges
be ween
60
up
o
100
Am2/kg
[37].
Thei
highe
con en
in
hese
samples
con ibu es
o
inc ease
in
magne iza ion.
The
same
endency
is
documen ed
in
Henkel
plo s
in
Fig.
9
ep esen ing
he
abo e
men ioned
o mula
M(H)
g aphically.
The
nega i e
dependences
documen
p e ailing
magne ic
dipola
(magne-
os a ic
dipole-dipole)
in e ac ions.
They
a e
p oduced
by
he
magne ic
momen
o
each
g ain
wi h
p e ailing
influence
o
he
Fe-oxides.
The
highes
peak
in ensi y
o
he
M(H),
−4.87
Am2/kg,
was
ob ained
o
he
ini ial
magne i e
(S1)
sam-
ple.
As
in
p e ious
obse a ions,
he
in ensi y
o
peaks
o
he
S5
and
S7
samples
abundan
in
magne i e
and
maghemi e
a e
highe
compa ed
o
he
o he
mixed
composi ions.
The
eason
o
hese
“anomalies”
is
unknown
in
his
momen .
I
can
be
only
specula ed
ha
i
could
come
o
an
un hough -o
condi ions
du ing
calcina ions
ea men .
The
Mössbaue
spec oscopy
was
applied
and
he
phases
and
hype fine
in e ac ions
analysed
o
comple e
mac oscopic
magne ic
p ope ies.
The
selec ed
Mössbaue
spec a
mea-
su ed
a
oom
empe a u e
a e
shown
in
Fig.
10.
The
spec a
j
m
a
e
e
s
e
c
h
n
o
l
.
2
0
2
0;9(3):4431–4439
4435
Fig.
4
–
Mo phology
as
seen
in
SEM,
seconda y
elec ons
(a)
and
XRD
di ac og am
(b)
o
ce ium
dioxide
ob ained
om
he
ce ium
ca bona e
a e
calcina ions’
ea men
a
500 ◦C/2
h/ai .
Table
1
–
Phase
composi ion
o
samples
de e mined
by
XRD
and
Mössbaue
phase
analysis
(MS,
only
e omagne ic
phases).
Nominal
composi ion
Sample
Me hod
Fe3O4␣-Fe2O3␥-Fe2O3␣-FeOOH
CeO2
w .%
Fe3O4S1 XRD
100.0
MS
74.5
18.7
5.0
Fe3O4/500 ◦C/2
h/ai S2 XRD
3.0
67.9
29.1
MS
8.1
66.8
22.6
1.7
CeO2(Ce2(CO3)3)/500 ◦C/2
h/ai S3 XRD
100.0
MS
Fe3O4+5
w .%
Ce2(CO3)3/500 ◦C/2
h/ai
S4 XRD
3.2
70.3
21.9
4.6
MS
9.8
66.3
21.0
1.5
Fe3O4+10
w .%
Ce2(CO3)3/500 ◦C/2
h/ai
S5 XRD
10.3
34.9
46.5
8.3
MS
14.9
45.4
36.5
2.7
Fe3O4+20
w .%
Ce2(CO3)3/500 ◦C/2
h/ai
S6 XRD
7.1
59.9
9.1
23.9
MS
10.2
66.3
19.6
2.1
Fe3O4+30
w .%
Ce2(CO3)3/500 ◦C/2
h/ai
S7 XRD
15.2
21.1
26.0
37.7
MS
13.8
41.1
40.2
3.0
Fe3O4+40
w .%
Ce2(CO3)3/500 ◦C/2
h/ai
S8 XRD
9.2
29.6
16.1
45.1
MS
11.1
55.6
28.3
2.0
Fe3O4+50
w .%
Ce2(CO3)3/500 ◦C/2
h/ai
S9 XRD
0.0
24.5
26.0
49.5
MS
12.7
51.5
30.8
2.8
Fig.
5
–
EDX
maps
o
cons i uen
elemen s
dis ibu ion
in
calcina ed
samples
wi h
nominal
composi ion
Fe3O4+10
w .%
Ce2(CO3)3(a)
and
Fe3O4+50
w .%
Ce2(CO3)3(b).

4436
j
m
a
e
e
s
e
c
h
n
o
l
.
2
0
2
0;9(3):4431–4439
Fig.
6
–
Pa icle
size
dis ibu ion
o
inpu
Fe-
and
Ce-oxides
(S1,
S3)
and
o
mixed
samples.
Fig.
7
–
Hys e esis
loops
o
he
ini ial
magne i e
(S1),
calcina ed
magne i e
(S2)
and
ce ium
ca bona e
(S3)
including
de ails
a
low
magne ic
fields.
o
S1,
S2,
and
mixed
S4
up
o
S9
samples
we e
e alua ed
wi h
a
se
o
Lo en zian
sex uple s
ep esen ed
e omagne ic
phases.
Besides
hem
also
he
double-line
componen s
we e
p esen
in
middle
o
all
samples
and
hey
a e
seen
also
in
spec a
p esen ed
in
Fig.
10.
Simila
spec a
a e
seen
and
discussed
in
Re .
[38].
In
case
o
he
S1
and
S2
samples
he
hype fine
pa ame e s,
ı
and
,
∼0.23
mm/s
and
0.35
mm/s,
o
Fig.
8
–
Dependence
o
magne ic
cha ac e is ics
on
olume
concen a ion
o
he
CeO2in
he
samples.
double-line
componen
can
be
asc ibed
o
Fe3+ ions.
In
he
mixed
samples
S4
up
o
S9
his
sub-componen
was
p esen
as
well
bu
ano he
pa amagne ic
componen
yielding
he
simila
hype fine
pa ame e
as
ob ained
o
ce ium
dioxide
in oduced
he eina e
was
de ec ed.
The
ep esen a ions
o
hese
componen s
we e
low
usually
a ound
1%.
The
spec um
o
ce ium
dioxide
(S3)
sample
was
fi ed
by
double-line
com-
ponen
wi h
he
isome
shi
ı
=
0.12
mm/s
and
quad upole
spli ing

=
0.58
mm/s
(86%)
and
single-line
componen
wi h
ı
=
0.25
mm/s
(14%)
which,
simila ly
as
in
p e ious
s udies
[30],
e iden ial
o
p esence
o
Fe-a oms.
The
e omagne ic
componen s
we e
i)
magne i e
ep e-
sen ed
by
alues
o
he
hype fine
induc ion
B
∼
48.6
T
and
∼
46.6
T,
o
he
isome
shi
ı∼
0.38
mm/s
and
∼
0.60
mm/s,
and
o
he
quad upole
spli ing

∼
−0.02
mm/s
and
∼
0.0
mm/s,
ii)
maghemi e
o
pa ame e s
B
∼
50.3
T,
ı
∼
0.27
mm/s,
and

∼
0.04
mm/s,
and
iii)
haema i e
B
∼
51.5
T,
ı
∼
0.37
mm/s,
and

∼
−0.18
mm/s.
These
Fe-oxide
phases
suppo
he
esul s
ob ained
abo e
by
XRD.
Ne e heless,
he
o he
componen
o
hype fine
pa ame e s
B
∼
41
T,
ı
∼
0.47
mm/s,
and

∼
−0.25
mm/s
was
de ec ed.
I
could
be
asc ibed
o
goe hi e.
The
ela i e
ep esen a ions
o
e omagne ic
phases
de ec ed
by
MS
a e
p esen
oge he
wi h
XRD
da a
in
Table
2.
The
j
m
a
e
e
s
e
c
h
n
o
l
.
2
0
2
0;9(3):4431–4439
4437
Fig.
9
–
Henkel
plo s
o
he
ini ial
(S1)
and
ea ed
(S2)
magne i e
and
he
mixed
Fe-oxide
wi h
a ious
con en
o
ce ium
dioxide
om
5
w .%
(S4)
up
o
50
w .%
(S9).
sligh
di e ences
in
alues
be ween
bo h
me hods
a e
due
o
highe
sensi i i y
o
Mössbaue
spec ome y
on
i on
con ain-
ing
phases
and
hei
o de ing.
3.3.
Deg ada ion
e ficiency
As
was
men ioned
abo e
a
sea ching
o
magne ically
sepa-
able
so ben s
is
in
p og ess
o
he
se e al
las
yea s.
He e,
he
deg ada ion
e ficiency
o
se
o
he
samples
wi h
a ying
ini ial
composi ions
o
magne i e/ce ium
ca bona e
and
cal-
cina ed
a
he
same
condi ions
was
es ed
o
he
deg ada ion
o
pa a hion
me hyl
(PM)
and
i s
con e sion
in o
4-ni o enol
(FN).
Du ing
his
chemical
p ocedu e
he
a e
o
chemical
eac-
ion
de e mines
he
dec easing
amoun
o
PM
and
inc easing
amoun
o
FN.
Bo h
componen s
can
be
measu ed
simul a-
neously.
This
eac ion
can
be
exp essed
by
simplified
ela ion
cPM =
cPM0 *
exp(−k* ),
whe e
k
is
a e
cons an
and
cPM0 is
he
ini ial
concen a ion
o
PM
compound
and
cPM is
concen a-
ion
o
PM
compound
a
ime
.
The
same
dependence
can
be
w i en
also
o
FN
componen .
The
changes
o
k
in
he
es ed
samples
a e
depic ed
in
Fig.
11.
I
seems
ha
cPM =
cFN is
alid
up
o
app oxima ely
25
ol.%
CeO2.
The
sligh
di e ences
obse ed
a
highe
CeO2con en s
can
imply
mo e
complica ed
eac ion.
I
appea s
also
ha
p esence
o
Fe-oxides
sligh ly
mode a e
he
a e
o
decomposi ion.
4.
Conclusions
P esen
in es iga ions
a e
de o ed
o
magne ically
sepa able
eac i e
so ben s
p epa ed
as
composi e
o
di e en
weigh
con en s
o
he
magne i e/ce ium
ca bona e
(100/0
up
o
50/50)
subjec ed
o
calcina ion
ea men s
a
500 ◦C
o
2
h
in
ai .
Fig.
10
–
Mössbaue
spec a
o
ini ial
(S1)
and
he mally
ea ed
(S2)
magne i e,
calcina ed
ce ium
ca bona e
(S3)
and
selec ed
mixed
samples
composed
o
Fe-oxide
and
o
30
w .%
(S7)
and
50
w .%
(S9)
ce ium
dioxide.
Va ious
cha ac e iza ion
expe imen al
me hods
ha e
e ealed
a
numbe
o
s uc u al
and
physical
aspec s.
The
main
conclusions
can
be
summa ised
subsequen ly.
•
Comme cial
magne i e
(Fe3O4)
con ains
also
small
amoun
o
maghemi e
and
␣-FeOOH
de ec ed
by
highly
sensi i e
Mössbaue
spec oscopy.
4438
j
m
a
e
e
s
e
c
h
n
o
l
.
2
0
2
0;9(3):4431–4439
Fig.
11
–
Deg ada ion
e ficiency
exp essed
as
he
a e
cons an
o
he
pa a hion
me hyl
decomposi ion
(PM,
•)
o
o
he
4-ni o enol
c ea ion
(FN,
o)
and
amoun
o
Fe-oxides
(夽)
in
dependence
o
CeO2con en
in
measu ed
samples.
•
Tempe a u e
ea men
(500 ◦C/2
h/ai )
o
magne i e
leads
o
he
ans o ma ion
in o
maghemi e
and
hema i e
and
dec eases
he
con en
o
␣-FeOOH.
•
All
hese
i on-oxides
a e
p esen
also
in
o he
samples
in
di e en
amoun s.
•
X- ay
di ac ion
o
ea ed
ce ium
ca bona e
(500 ◦C/2
h/ai )
confi ms
i s
ans o ma ion
in o
ce ium
oxide
o
he
fluo i e-like
c ys alline
s uc u e
and
flake- o m.
•
X- ay
di ac og am
analysis
yields
sligh ly
di e en
CeO2
con en
compa ed
o
nominal
one.
•
Di e ences
be ween
XRD
and
Mössbaue
esul s
in
ep-
esen a ion
o
indi idual
phases
a e
due
o
dissimila
sensi i i y
o
bo h
expe imen al
me hods.
•
Dispe sion
in
mic o-domain
and
pa icle
size
da a
despi e
he
same
ea ed
pa ame e s
o
all
samples
(500 ◦C/2
h/ai )
imply
ha
mo e
a en ion
should
be
done
o
condi ions
o
sample
p epa a ion
and
o
hei
subsequen
ea men .
•
Magne ic
cha ac e is ics,
sa u a ion
and
emanen
magne-
iza ions,
a e
de e mined
by
ype
and
con en
o
i on-oxide.
While
magne i e
(Ms
=
90÷100
Am2/kg)
and
maghemi e
(Ms
=
60÷80
Am2/kg)
a e
e imagne ic
wi h
only
sligh
di -
e ence
in
Ms
a
oom
empe a u e,
haema i e
is
weakly
e omagne ic
(Ms
∼
0.3
Am2/kg)
and
i s
highe
con en
in
he
samples
(S2,
S4,
S6,
S8,
S9)
con ibu es
o
he
lowe
alue
o
Ms.
Hype fine
induc ion
alues
(B)
a e
compa able
o
all
h ee
Fe-oxides
and
no
impo an
di e ences
among
sam-
ples
a e
he e o e
isible.
•
The
deg ada ion
e ficiency
seems
o
be
independen
on
ype
o
i on-oxide
bu
inc eases
wi h
con en
o
ce ium
dioxide.
•
Insu ficiency
o
p esen
s udies
is
ha
no
in o ma ion
con-
ce ning
ce ium
dioxide
was
ob ained
in
despi e
o
a ious
expe imen al
me hods.
Some
s udies
o
o he
au ho s
show
ha
ce ium
dioxide
can
con ain
besides
dominan
dia-
magne ic
Ce4+ ions
also
pa amagne ic
Ce3+ ions
mainly
a
pa icle
su aces
due
o
acancy- ype-de ec
o ma ion.
The
a io
o
Ce4+ and
Ce3+ ions
could
con ibu e
o
be e
expla-
na ion
o
he
deg ada ion
e ficiency.
Conflic s
o
in e es
The
au ho s
decla e
no
conflic s
o
in e es .
Acknowledgemen s
The
au ho s
hank
M.
Dosek
om
he
Facul y
o
En i onmen ,
Uni e si y
J.E.
Pu kyne
o
his
help
wi h
sample
p epa a-
ion.
This
wo k
was
unded
by
he
Czech
Science
Founda ion
ia
he
p ojec
No.
19-07460S
and
by
Minis y
o
Educa ion
You h
and
Spo s
o
he
Czech
Republic
ia
he
ollow-
ing
p ojec s:
No.
CZ.02.1.01/0.0/0.0/17
048/0007399
(ERDF/ESF
New
Composi e
Ma e ials
o
En i onmen al
Applica ions),
No.
LQ1601
(CEITEC
2020-Na ional
Sus ainabili y
P og amme
II),
ID
LM2015041
(CEITEC
Nano
Resea ch
In as uc u e),
No.
CZ.1.05/2.1.00/19.0387
(De elopmen
o
he
Resea ch
and
De elopmen
Base
o
RMSTC),
and
No.
2015073
(NanoEn iCz
Resea ch
In as uc u e).
Appendix
A.
Supplemen a y
da a
Supplemen a y
ma e ial
ela ed
o
his
a icle
can
be
ound,
in
he
online
e sion,
a
doi:h ps://doi.o g/10.1016/j.
jm .2020.02.068.
e
e
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