Hydrothermal synthesis of nano bilayered v2o5 and electrochemical behavior in non–aqueous electrolytes lipf6 and naclo4
In summary, we had synthetized nano–crystalline bilayered V2O5 by hydrothermal rout
from a precursor of VCl3. The XRD pattern of bilayered V2O5 showed the typical (00l) with an
interlayer spacing of 11.7 Å. Bilayered V2O5 could insert reversiblely 1.5 ion Li+ (~220 mAh/g);
while a stability of sodium’s intercalation occurred at 0.8 ion, corresponding to a specific
capacity of 120 mAh/g. The sodium diffusion coefficients were found around 10–11 cm2/s, This
value is lower 100 times than the lithium diffusion coefficients (~10–9 cm2/s) due to a larger
ionic radius of sodium ion.
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Journal of Science and Technology 55 (1B) (2017) 24–29
HYDROTHERMAL SYNTHESIS OF NANO BILAYERED V2O5
AND ELECTROCHEMICAL BEHAVIOR IN NON–AQUEOUS
ELECTROLYTES LiPF6 AND NaClO4
Huynh Le Thanh Nguyen1, *, Nguyen Van Hoang2, Nguyen Thi Ngoc Dieu1,
Huynh Bang Vy1, Le My Loan Phung1, 2, Tran Van Man2
1Applied Physical Chemistry Laboratory, Faculty of Chemistry,
University of Science–VNUHCM, 227 Nguyen Van Cu, District 5, Ho Chi Minh City, Vietnam
2Department of Physical Chemistry, Faculty of Chemistry, University of Science–VNUHCM
227 Nguyen Van Cu, Ward 4, District 5, Ho Chi Minh City, Vietnam
*Email: hltnguyen@hcmus.edu.vn
Received: 30 December 2016; Accepted for publication: 2 March 2017
ABSTRACT
This work aimed to prepare bilayered V2O5 by hydrothermal route from vanadium (III)
chloride (VCl3). According to XRD results, bilayered V2O5 showed a large interlayer spacing
around 11.3 Å. The electrochemical properties of bilayered V2O5 were carried out by cyclic
voltammetry and charge–discharge testing in non–aqueous electrolytes LiPF6 and NaClO4. The
curves charge–discharge showed that mechanism of insertion/extraction of Li+ ions and Na+ ions
were occurred on a solution solid without the phase transition. Moreover, specific capacity for
lithium and sodium intercalation of bilayered V2O5 were found out 250 mAh/g and 200 mAh/g,
respectively. The kinetic of lithium’s and sodium’s insertion was evaluated by the
electrochemical impedance spectroscopy (EIS). The EIS results exhibited a stabilization of
charge transfer in both case and a slow kinetic of sodium’s diffusion compared to lithium’s case
due to the large ionic radius of sodium.
Keywords: electrochemical impedance spectroscopy, kinetics, lithium’s intercalation, sodium’s
intercalation, bilayered V2O5.
1. INTRODUCTION
In 21th century, rechargeable batteries are main key of modern technology in many
applications from portable devices (smartphone, laptop) to large–scale (hydride electric
vehicle–HEV, smart grid system) [1–3]. Among the rechargeable batteries, Li–ion battery
(LIB) is outstanding member due to the highest gravimetric as well as volumetric capacity; and
Sodium–ion batteries (SIBs) can have contribution to alternating LIBs in large–scale application.
Li–ion and Na–ion batteries have the same configuration with an insertion/extraction reversible
of Li+ ions and Na+ ions into electrode positive and negative during charge–discharge process [4,
5].
Huynh Le Thanh Nguyen, et al.
25
Bilayered V2O5 is a promising cathode material for both Li–ion and Na–ion batteries
because of a large interlayer spacing around 10 Å [6, 7]. In this work, we investigate the
insertion electrochemical of Li+ ion and Na+ ion into bilayered V2O5 in non–aqueous electrolyte.
Moreover, a comparison of kinetics of lithium–sodium intercalation into nano crystalline V2O5
bilayered was carried out. The electrochemical impedance spectroscopy results exhibited the
slow kinetics of sodium intercalation compared to lithium intercalation due to the large ionic
radius of sodium.
2. MATERIALS AND METHODS
Bilayered V2O5 were prepared by a hydrothermal route. A mixture of 1 mmol of VCl3
(Sigma–Aldrich, 97 %), 5 mL pyridine (Sigma–Aldrich) and 10 mL deionized water was stirred
under vigorous at room temperature. After that, the precursor solution was heated at 180 °C in a
teflon–lined autoclave for 12 hours. The precipitate was cooled to room temperature naturally,
collected, and washed with deionized water and ethanol several times. The final products were
obtained after drying at 120 °C in a vacuum oven overnight. Structures of these samples were
identified by powder X–ray diffraction, using a X’Pert PRO MPD PANalytical diffractometer
(at Center for Innovative Materials and Architectures, Ho Chi Minh City) with CoKα radiation
(λ = 1.789 Å), 0.02° and 20 second pars step counting time. The diffraction pattern was collected
for 2θ between 10° to 70°. The morphology and the distribution of grain size were determined
by using a FE–SEM S4800 (Hitachi, Japan) at Institute of Chemical Technology–VAST.
The electrochemical properties were measured in a Swagelok–type cell. The positive
electrode was composed on material active (80 wt%), acetylene black (7.5 wt%), graphite
(7.5 wt%) and teflon (5 wt%). The mixture was pressed directly on a stainless–steel grid under a
pressure of 5 ton/cm2. Negative electrode was lithium or sodium metal and 1 M LiPF6/ethylene
carbonate:dimethyl carbonate or 1 M NaClO4/propylene carbonate (2 % fluoroethylene
carbonate) were used as electrolyte, respectively. Cells were assembled in a glove box under
argon to avoid oxygen and water. The kinetic of insertion–extraction of lithium or sodium into
bilayered V2O5 were investigated by using electrochemical impedance spectroscopy. Impedance
measurements were performed in the frequency range from 106 Hz to 5×10–3 Hz. The excitation
signal was 10 mV peak to peak. Electrochemical studies were carried out by using VMP3
apparatus (BioLogic–France). All electrochemical characterizations were implemented at
Faculty of Chemistry, University of Science–VNUHCM.
3. RESULTS AND DISCUSSION
3.1. Structure and morphology
The bilayered V2O5, called V2O5.nH2O xerogel, is a stack of long ribbon like slabs which
are made up of octahedral [VO6] stacked along c–axis, as shown in Figure 1a with a distance
inter–layer of 11.5 Å [8–10]. The XRD pattern of bilayered V2O5 (Figure 1b) showed the typical
(00l) refection peaks, which are consistent with those of the layered structure of V2O5.nH2O
(JCPDF: 40–1296). According to XRD pattern, the distance interlayer was determined to 11.7 Å.
Due to the hydrothermal reaction, the peaks in XRD pattern had quite large. It is considered
that the sample was crystallized in small particle sizes. According to the Debye–Scherrer
equation (1), the average size of particles was calculated from the full width of half maximum
(FWHM) of diffraction peaks:
Hy
26
wh
wa
is t
fas
dif
dis
aro
3.2
bil
wh
int
(ex
1 M
dis
drothermal s
ere dhkl is th
velength of
he diffractio
t kinetic of
fusion.
As can b
tribution, an
und 1 μm.
. Electroche
During ch
ayered V2O5
ere A+ may
ercalation (
traction, cha
Figure 3a
LiPF6/EC
charge curv
ynthesis of
e average si
CoKα X–ray
n angle. Th
intercalatio
e seen in
d the particl
Figure 1.
mical prop
arge–discha
occur follow
represent a
insertion, d
rge). Interca
showed the
:DMC (1:1)
es showed a
nano bilayer
ze, k is the
radiation (
e size reache
n of lithiu
Figure 2,
e size fell in
Structure of b
Figure 2. S
erties
rge process
ing electro
V2O5
monovalent
ischarge), w
lation and d
typical cha
solution at w
totally reve
ed V2O5 and
ࢊࢎ ൌ ࢼࢉ
constant dep
1.789 Å), β
d around 20
m and sodi
the sample
to the micro
ilayered V2O
EM images o
, the inserti
chemical rea
+ xA+ + xe–
cation (Li+ a
hile the b
eintercalatio
rge–discharg
indow pot
rsible interc
electrochem
ࣅ
࢙ࣂ
ending on th
is the FWHM
nm. The na
um ion due
bilayered V
metric dime
5 and XRD p
f bilayered V
on/extraction
ction:
↔ AxV2O5
nd Na+). He
ackward rea
n proceed re
e curves of
ential 1.5–4.
alation of L
ical behavio
e crystallite
of the mos
nosize of pa
to shorten
2O5 had a
nsion scale.
attern of samp
2O5.
of Li+ ion
re, the forw
ction is ter
versibly in o
bilayered V
2 V (vs. Li+
i+ ions. In t
i r in non–aq
shape (0.9)
t intense pe
rticles will
ing the pat
homogeno
The particle
le.
s and Na+
ard reaction
med deinte
pposite dire
2O5 in non–
/Li). All the
he 1st cycle,
ueous
(1)
, λ is the
ak, and θ
suggest a
hway of
us grain
size was
ions into
is called
rcalation
ctions.
aqueous
charge–
the host
cou
Mo
un
per
mA
1 M
irr
1st
str
wi
ins
int
4b
3.3
im
fre
ld insert 1
reover, the
complicated
formance w
h/g.
Figure 3
Figure 4a
NaClO4/P
eversible ins
reduction b
uctural of b
th an electro
ertion of so
eraction of N
; after thirty
Figure 4. (
. Kinetic of
Kinetics o
pedance sp
quency rang
.5 Li+ ions
curves repr
insertion
as presented
. (a) Typical
showed the
C (2 % FEC
ertion of Na
ut only 0.9
ilayered V2O
chemically
dium ions.
a+ ions and
cycles, a spe
a) Typical cha
lithium’s an
f alkaline io
ectroscopy
e 105 Hz
, correspond
esent a low
of Li+ ions
in Figure 3
charge–discha
1 M
typical cha
) solution a
+ ions were o
Na+ ions co
5 and α–V2
formed phas
All the curv
bilayered st
cific capacit
rge–discharg
NaC
d sodium’s
n’s transpor
method. Th
to 5×10–3 H
ing to a m
polarization
with a m
b; after fifte
rge curves an
LiPF6/EC:D
rge–discharg
t window p
bserved, bil
uld extract
O5. In α–V2
e α’–NaV2O
es showed
ructure. The
y reduced to
e curves and (
lO4 1 M/PC (
intercalati
t into bilaye
e impedan
z at a vari
aximum sp
as well as
echanism
en cycles, a
d (b) cycling
MC (1:1).
e curves of
otential 1–4
ayered V2O
in oxidation
O5 case, the
5 [11]. In 2
a large pola
cycling perf
100 mAh/g
b) cycling pe
2 % FEC).
on
red V2O5 wa
ce measure
ous content
Huynh Le
ecific capa
a simply fo
of solution
specific cap
performance
bilayered V
V (vs. Na+
5 could inser
. This result
sodium's in
nd cycle, we
rization tha
ormance wa
.
rformance of
s determine
ments were
of alkaline
Thanh Nguy
city of 230
rm that ind
solid. The
acity reduce
of bilayered V
2O5 in non–
/Na). In 1st
t 1.35 Na+ io
exhibited a
sertion acco
observe a r
t suggested
s presented
bilayered V2O
d by electro
performed
ion. The
en, et al.
27
mAh/g.
icates an
cycling
d to 150
2O5 in
aqueous
cycle, an
ns in the
relation
mpanied
eversible
a strong
in Figure
5 in
chemical
in the
diffusion
Hy
28
co
[12
wh
(0.
rel
in
fre
res
rea
an
dif
0,1
co
(Fi
lith
0.0
dis
we
drothermal s
efficients of
]:
ere, VM is t
785 cm2); │
ation betwee
For lithiu
the high–m
quency f* =
istance of ch
l axis demo
gle was incre
fusion allow
and DLi = 8
efficients in
In case o
gure 6). How
ium’s case,
2 Hz). It co
charge proc
re found DN
ynthesis of
alkaline ion
he molar vo
dE/dx│ is t
n ZReal and ω
m’s intercal
edium freq
63 Hz. An u
arge transfe
nstrated the
asing which
ed to calcul
.9×10–9 cm2
α–V2O5 and
F
F
f sodium’s
ever, the “
and the Wa
uld be expla
ess and a la
a = 9.5×10–1
nano bilayer
D were ca
ࡰࡸ/ࡺ
lume of host
he slope at f
–1/2 in the W
ation, the di
uency corre
nchanged ch
r”. The low
Warburg im
belonged to
ate the lithi
/s for xLi = 0
bronzes MxV
igure 5. AC i
igure 6. AC i
intercalatio
quasi–resista
rburg region
ined by the
rger ionic r
1 cm2/s for x
ed V2O5 and
lculated from
ࢇ ൌ ቀ ࢂࡹ√ࡲࡿ ൈ
(VM = 54.5
ixed x and d
arburg imp
agram impe
sponded to
aracteristic
frequency r
pedance and
the finite d
um diffusion
.4. These va
2O5.
mpedance di
mpedance dia
n, the diag
nce of char
in sodium
passivation
adius of so
Na = 0.1 and
electrochem
region Wa
ࢊࡱ
ࢊ࢞ ൈ
࣓ቁ
cm3/mol); S
etermined b
edance.
dance presen
the charg
frequency p
egion, a stra
at lower fre
iffusion proc
coefficient
lues were co
agrams for Li
grams for Na
ram impeda
ge transfer”
’s case was
and evolutio
dium ion. T
DNa = 1.2×1
ical behavio
rburg by fo
is the active
y curve C/6
ted three re
e transfer w
roposed a sta
ight line 45°
quencies (f
ess (Figure
s: DLi = 1.3
herent with
0.1V2O5.
0.1V2O5.
nce exhibit
in sodium’s
found at low
n of sodium
he sodium d
0–11 cm2/s fo
i r in non–aq
llowing equ
surface of
0, Aω is the
gions. A sem
ith a char
bilization o
(1–0.1 Hz)
< 10–3 Hz) t
5). The sem
×10–9 cm2/s
the lithium
ed the sam
case was la
er frequenc
’s surface d
iffusion co
r xNa = 0.4.
ueous
ation (2)
(2)
electrode
slope of
i–circle
acteristic
f “quasi–
from the
he phase
i–infinite
for xLi =
diffusion
e model
rger than
ies (0.4–
uring the
efficients
Huynh Le Thanh Nguyen, et al.
29
4. CONCLUSIONS
In summary, we had synthetized nano–crystalline bilayered V2O5 by hydrothermal rout
from a precursor of VCl3. The XRD pattern of bilayered V2O5 showed the typical (00l) with an
interlayer spacing of 11.7 Å. Bilayered V2O5 could insert reversiblely 1.5 ion Li+ (~220 mAh/g);
while a stability of sodium’s intercalation occurred at 0.8 ion, corresponding to a specific
capacity of 120 mAh/g. The sodium diffusion coefficients were found around 10–11 cm2/s, This
value is lower 100 times than the lithium diffusion coefficients (~10–9 cm2/s) due to a larger
ionic radius of sodium ion.
Acknowledgements. This work was supported by University of Sciences (VNU–HCMC) through grant
T2016–23 and by Vietnam National University of Ho Chi Minh City through grant NVTX–2017.
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