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Short Communication
Effect of zirconium oxide nanoparticles on surface
morphology and energy storage of electrochemical capacitors
Mahdi Nasibi a,b,n
, Mahdi R. Sarpoushi a
, Rouhallah Hesan c
,
Mohammad Ali Golozar d
, Masoud Moshrefifar c
a
Technical Inspection Engineering Department, Petroleum University of Technology, Abadan, Iran
b
Health and Safety Engineering (HSE) Office, NIOPDC, Yazd Region, Yazd, Iran
c
Materials and Mining Engineering Department, Yazd University, Yazd, Iran
d
Materials Science and Engineering Department, Isfahan University of Technology, Isfahan, Iran
a r t i c l e i n f o
Keywords:
Supercapacitors
Nanomaterials
Morphology
ZrO2
a b s t r a c t
In this study, the effect of mixing zirconium oxide nanoparticles and carbon black particles
on surface morphology and electrochemical performance of prepared electrodes were
investigated. Scanning electron microscopy was used to characterize microstructure and
nature of nanocomposites. Charge stored (q) on different nanoparticle containing
electrodes was calculated and the effect of surface morphology on charge storage was
discussed. It is concluded that charge stored on the electrode shows an n-like change by
increasing nanoparticle content of electrodes. Addition of nanoparticle increases qn
O/qn
T
(from 0.05 to 0.18) which confirms the higher current response and higher voltage
reversal at the end potentials.
Crown Copyright & 2014 Published by Elsevier Ltd. All rights reserved.
1. Introduction
Electrochemical capacitors (ECs), with a combination of
high power density and high energy density, can be used
as a complementary energy-storage device along with a
primary power source, such as a battery or a fuel cell, for
power enhancement in short pulse applications [1]. High
cycle life, high energy efficiency and high self-discharge
rate are some of the supercapacitors characteristics [2,3].
Today, many laboratories are actively engaged in develop-
ment of well-known type of supercapacitors, viz., electro-
chemical double-layer, pseudo and hybrid supercapacitors,
and most research has been focused on development of
different electrode materials [4,5]. For practical applica-
tions, an EC must fulfill the following technical require-
ments: high specific capacitance, long cycle life and
high charge/discharge rate. Today, using nanoparticles is
of interest in order to improve these parameters. So,
nanoparticles distribution quality on the electrode surface
is of most important parameters [6]. In our previous work,
we investigated the effect of different mixing processes of
electrode material on dispersion quality of nanoparticles
which change their electrochemical performance. In this
work, we investigate the effect of nanoparticle contents of
the electrode material on microstructure and nature of
prepared electrodes using scanning electron microscopy,
and potentiodynamic polarization techniques. At the
end, quantitative measurements were reported for further
investigations.
2. Experimental
2.1. Materials
High purity (499%) nano-sized zirconium oxide (ZrO2)
particles (o100 nm), nickel foil (99.99% with 0.125 mm
Contents lists available at ScienceDirect
journal homepage: www.elsevier.com/locate/mssp
Materials Science in Semiconductor Processing
http://dx.doi.org/10.1016/j.mssp.2014.03.037
1369-8001/Crown Copyright & 2014 Published by Elsevier Ltd. All rights reserved.
n
Corresponding author. Tel.: þ98 9113708480; fax: þ98 6314423520.
E-mail address: mahdi.nasibi@gmail.com (M. Nasibi).
Materials Science in Semiconductor Processing 24 (2014) 260–264
thickness) and polytetrafluoroethylene (o2 μm) were
purchased from Aldrich, USA. All other chemicals used in
this study were purchased from Merck, Germany. Carbon
black particles (o2 μm) were purchased from Degussa,
Germany. In order to prepare electrodes, the mixture
containing different wt% ZrO2 and carbon black (CB) and
10 wt% polytetrafluoroethylene (PTFE) was well mixed in
ethanol to form a paste and then was pressed onto the
nickel foil (25 MPa), which served as a current collector
(surface was 0.785 cm2
). The typical mass weight of
electrode material was 30 mg. The used electrolyte was
2 M KCl.
2.2. Characterization
The electrochemical measurements were performed
using an Autolab (Netherlands) potentiostat Model
PGSTAT 302N. CV tests were conducted at various scan
rates (s) with recording of potential response currents, I,
which is related by C¼I/s where C is the capacitance of the
electrode interface. The specific capacitance C (FgÀ1
) of the
active material was determined by integrating either the
oxidative or reductive parts of the cyclic voltammogram
curve to obtain voltammetric charge Q (C). This charge was
divided by mass of active material m (g) in the electrode
and width of the potential window of the cyclic voltam-
mogram ΔE (V), i.e., C¼Q/(ΔEm) [7]. The morphology and
nature of the prepared electrodes were studied using
scanning electron microscopy (TESCAN, USA).
3. Results and discussion
Nanoparticles distribution quality on the electrode
surface is one of the key parameters which controls the
electrical performance of nanoparticle containing electro-
des for supercapacitors. Using macroparticles like used
carbon black particles which store electrical energy
through the double layer mechanism, will make macro-
pores and macrogrooves with deep and hollow shapes on
surface of the electrode. Using the nanoparticles will make
nanopores with shallow shapes. Therefore, mixing the
nanoparticles with macroparticles will have a significant
effect on the morphology and nature of the prepared
electrodes. One of the thinkable morphology changes
by mixing of the nanoparticles with macroparticles is
schematically illustrated in Fig. 1. In the absence of the
nanoparticles, macrogrooves produced between CB parti-
cles and these grooves are exposed to the electrolyte for
charge storage (Fig. 1(a)). As the nanoparticle content of
Fig. 1. (a–d) Schematic illustration of the surface changes by addition of
nanoparticles into the electrode material and, (e) SEM image obtained
from 30:60:10 electrode. (For interpretation of the references to color in
this figure, the reader is referred to the web version of this article.)
Fig. 2. Nyquist diagrams of different ZrO2-content electrodes in 2 M KCl
electrolyte.
M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264 261
the electrodes increases the macropores are filled with
nanoparticles and the depth of the macrogrooves are
decreased (Fig. 1(b) and (c)). Then, all grooves are filled
and the CB particles on the surface of the electrode are
covered with a thin layer of ZrO2 nanoparticles and finally,
macrogrooves are replaced with the nanoporous structure
prepared by the nanoparticles (Fig. 1(d)). Therefore, active
surface used for charge storage on the surface of the
electrode is replaced and this increases the specific surface
area of the prepared electrodes. SEM images obtained from
30:60:10 (CB:ZrO2:PTFE) electrodes (Fig. 1(e)) confirm the
presence of macrogrooves made between the CB particles
(were shown by red lines) which nearly filled with ZrO2
nanoparticles. In these electrodes, CB particles can provide
a conductive channel due to their excellent conductivity.
Unlike the CB particles, metal oxides like ZrO2 are low
conductive materials but, have a pseudo capacitive char-
acteristic which can take place in redox reactions and
improve the energy storage capability of the electrodes.
This low conductivity decreases the charge stored on the
electrodes, especially at high sweep rates. Therefore, as the
nanoparticle content of the electrode increases, it is
proposed that the total charge stored on the electrode
surface increases, at first, due to increasing the specific
surface area and changing the charge storage mechanism
from double layer to pseudo, and then decreases due to
increasing the electrical resistance of the electrode.
The principle reaction involved in the charging and
discharging processes of zirconium dioxide in an aqueous
electrolyte can be described by reaction (1)
ZrIV
O2 þλþ
þeÀ
2ZrIII
OOλ ð1Þ
where λ denotes Kþ
, Hþ
.
Additionally, two mechanisms can be proposed for
supercapacitive charge storage in ZrO2. The first mechan-
ism is based on the intercalation/extraction of protons or
Fig. 3. Capacitance vs. potential curves obtained from (a) 90:00:10, (b) 50:40:10, (c) 30:60:10, (d) 20:70:10 and (e) 10:80:10 electrodes in 2 M KCl electrolyte.
M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264262
alkali cations into the oxide particles (denoted as reaction
(2)), whereas the second mechanism involves the surface
adsorption/desorption of proton or alkali cations probably
(denoted as reaction (3)):
ZrO2 þMþ
þeÀ
¼ ZrOOM ð2Þ
and
ðZrO2Þsurface þMþ
þeÀ
¼ ðZrOOMÞsurface ð3Þ
where Mþ
denotes Kþ
or H3Oþ
.
In order to gain a quantitative information on the effect of
surface changes on charge storage mechanism of the ZrO2/CB
electrodes by increasing the nanoparticle content of the
electrodes, the voltammograms obtained from different
nanoparticle containing electrodes were analyzed as a func-
tion of scan rate, according to the procedure reported by
Ardizzone et al. [8]. Then, the total charge and charge related
to the most accessible surface area were calculated.
Four prominent characteristics can be reported by chan-
ging the nanoparticle content of the electrodes from
obtained CV curves (Fig. 3): changing the shape of the CV
curves, changing the specific capacitance, deviation of the CV
curves from the classical square waveform expected for a
pure capacitor by increasing the sweep rate and, increasing
the voltage reversal at end potentials. As the nanoparticle
content of the electrodes increases electrical resistance of the
electrode increases (Fig. 2) and, up to 60%, the energy stored
on the electrode increases at first and then decreases due to
the electrical resistance and specific surface area changes of
the electrodes. Additionally, scan rate dependence of the
capacitance can be related to the less accessible surface area
(pores, cracks, etc) which become excluded as the rate
reaction is enhanced [9,10]. Ion diffusion ability of the
electrolyte into the surface of the electrode will have a
significant effect on the voltage reversal of the electrodes.
Improvement of the voltage reversal of the high nanoparticle
containing electrodes may be related to surface morphology
changes which change the active energy storage sites from
down the deep macropores to shallow nanopores. Calculat-
ing the total charge stored on electrodes and the charge
stored on less and more accessible surface area of the
electrodes are efficient indicators which indicate the charge
distribution on the electrode. In charge and discharge cycles,
the total charge can be written as a sum of an inner charge
from the less accessible reaction sites and an outer charge
from the more accessible reaction sites, i.e., q*
T¼q*
I þq*
O,
where q*
T, q*
I and q*
O are the total charge and charges related
to the inner and the outer surfaces, respectively [11]. The
extrapolation of q*
to v¼0 from 1/q*
vs. v1/2
plots obtained
from different nanoparticle containing electrodes (Fig. 4(a))
give the total charge qT which is the charge related to the
entire active surface of the electrode. In addition, extrapola-
tion of q*
to v¼1 (vÀ1/2
¼0) from the q*
vs. vÀ1/2
plots (Fig.
4(b)) give the outer charge q*
O, which is the charge due to
redox process on the most accessible active surface [8,11].
Total and outer charges vs. nanoparticle content of the
electrode obtained from different nanoparticle electrodes
were plotted in Fig. 4(c). Total and outer charge plots confirm
that the addition of nanoparticles increases and then
decreases the charge stored on the electrode surface, as
expected and explained above. Although, electrodes which
contain higher nanoparticle contents show higher ratio of the
outer charge to total charge (q*
O/q*
T) (increases from 0.05 to
0.18) which confirms the higher current response on voltage
reversal of high nanoparticle containing electrodes. Finally, it
is concluded that the 40:50:10 (CB:ZrO2:PTFE) electrodes
show better charge storage capability ($57C gÀ1
cmÀ2
)
(Fig. 4(c)). It may be due to the synergistic effect of the double
layer characteristic of the CB particles and the pseudo
characteristic of the ZrO2 nanoparticles. Changing the surface
morphology from macrogrooves to nanoporous structure
makes the 10:80:10 electrode to show the high outer charge
to total charge (q*
O/q*
T) ratio of as-high-as 0.18 which confirms
its high current response on voltage reversal.
4. Conclusions
In this study, effect of nanoparticle content of the ZrO2/
carbon black nanocomposite electrodes on the microstruc-
ture, nature and the electrochemical performance of the
prepared electrode were investigated. SEM images confirm
Fig. 4. (a) Extrapolation of q to v¼0 from the qÀ1
vs. v0.5
plot given the
total charge and (b) extrapolation of q to v¼1 from the q vs. vÀ0.5
plot
given the outer charge for CB electrodes. (c) Total and outer charge stored
on the different nanoparticle containing electrodes.
M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264 263
the surface changes from hallow macrogrooves to shallow
nanoporous structure by increasing the nanoparticle content
of the electrodes. Charge stored on the electrode surface
increases ($57C gÀ1
cmÀ2
obtained from 40:50:10 elec-
trode) at first, due to the synergistic effect of the carbon
black and ZrO2 nanoparticles, and then decreases by increas-
ing the nanoparticle content due to the electrical resistance
of the electrode. Finally, it is concluded that the current
response of the electrodes (q*
O/q*
T ratio of 0.18 obtained from
10:80:10 electrode) increases by addition of the nanoparti-
cles due to the surface changes from hollow macrogrooves to
the nanoporous structure.
References
[1] W. Wei, X. Cu, W. Chen, D.G. Ivey, J. Power Sources 186 (2009)
543–550.
[2] R. Kotz, M. Carlen, Electrochim. Acta 45 (2000) 2483–2498.
[3] I. Hadjipaschalis, A. Poullikkas, V. Efthimiou, Renew. Sustain. Energy
Rev. 13 (2009) 1513–1522.
[4] Y. Zhang, H. Feng, X. Wu, L. Wang, A. Zhang, T. Xia, Int. J. Hydrog.
Energy 34 (2009) 4889–4899.
[5] B.E. Conway, Electrochemical Capacitors Scientific Fundamental and
Technological Applications, Klumer Academic/Plenum, New York,
1999, 105–124.
[6] B. Babakhani, D.G. Ivey, J. Power Sources 195 (2010) 2110–2117.
[7] G. Sun, W. Song, X. Liu, W. Qiao, D. Long, L. Ling, Mater. Lett. 65
(2011) 1392–1395.
[8] S. Ardizzone, G. Fregonara, S. Trasatti, Electrochim. Acta 35 (1990)
263–267.
[9] B.E. Conway, W.G. Pell, J. Power Sources 105 (2002) 169–181.
[10] M. Nasibi, M.A. Golozar, Gh. Rashed, Mater. Lett. 91 (2013) 323–325.
[11] M. Nasibi, M.A. Golozar, Gh. Rashed, Mater. Lett. 85 (2012) 40–43.
M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264264

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  • 1. Short Communication Effect of zirconium oxide nanoparticles on surface morphology and energy storage of electrochemical capacitors Mahdi Nasibi a,b,n , Mahdi R. Sarpoushi a , Rouhallah Hesan c , Mohammad Ali Golozar d , Masoud Moshrefifar c a Technical Inspection Engineering Department, Petroleum University of Technology, Abadan, Iran b Health and Safety Engineering (HSE) Office, NIOPDC, Yazd Region, Yazd, Iran c Materials and Mining Engineering Department, Yazd University, Yazd, Iran d Materials Science and Engineering Department, Isfahan University of Technology, Isfahan, Iran a r t i c l e i n f o Keywords: Supercapacitors Nanomaterials Morphology ZrO2 a b s t r a c t In this study, the effect of mixing zirconium oxide nanoparticles and carbon black particles on surface morphology and electrochemical performance of prepared electrodes were investigated. Scanning electron microscopy was used to characterize microstructure and nature of nanocomposites. Charge stored (q) on different nanoparticle containing electrodes was calculated and the effect of surface morphology on charge storage was discussed. It is concluded that charge stored on the electrode shows an n-like change by increasing nanoparticle content of electrodes. Addition of nanoparticle increases qn O/qn T (from 0.05 to 0.18) which confirms the higher current response and higher voltage reversal at the end potentials. Crown Copyright & 2014 Published by Elsevier Ltd. All rights reserved. 1. Introduction Electrochemical capacitors (ECs), with a combination of high power density and high energy density, can be used as a complementary energy-storage device along with a primary power source, such as a battery or a fuel cell, for power enhancement in short pulse applications [1]. High cycle life, high energy efficiency and high self-discharge rate are some of the supercapacitors characteristics [2,3]. Today, many laboratories are actively engaged in develop- ment of well-known type of supercapacitors, viz., electro- chemical double-layer, pseudo and hybrid supercapacitors, and most research has been focused on development of different electrode materials [4,5]. For practical applica- tions, an EC must fulfill the following technical require- ments: high specific capacitance, long cycle life and high charge/discharge rate. Today, using nanoparticles is of interest in order to improve these parameters. So, nanoparticles distribution quality on the electrode surface is of most important parameters [6]. In our previous work, we investigated the effect of different mixing processes of electrode material on dispersion quality of nanoparticles which change their electrochemical performance. In this work, we investigate the effect of nanoparticle contents of the electrode material on microstructure and nature of prepared electrodes using scanning electron microscopy, and potentiodynamic polarization techniques. At the end, quantitative measurements were reported for further investigations. 2. Experimental 2.1. Materials High purity (499%) nano-sized zirconium oxide (ZrO2) particles (o100 nm), nickel foil (99.99% with 0.125 mm Contents lists available at ScienceDirect journal homepage: www.elsevier.com/locate/mssp Materials Science in Semiconductor Processing http://dx.doi.org/10.1016/j.mssp.2014.03.037 1369-8001/Crown Copyright & 2014 Published by Elsevier Ltd. All rights reserved. n Corresponding author. Tel.: þ98 9113708480; fax: þ98 6314423520. E-mail address: mahdi.nasibi@gmail.com (M. Nasibi). Materials Science in Semiconductor Processing 24 (2014) 260–264
  • 2. thickness) and polytetrafluoroethylene (o2 μm) were purchased from Aldrich, USA. All other chemicals used in this study were purchased from Merck, Germany. Carbon black particles (o2 μm) were purchased from Degussa, Germany. In order to prepare electrodes, the mixture containing different wt% ZrO2 and carbon black (CB) and 10 wt% polytetrafluoroethylene (PTFE) was well mixed in ethanol to form a paste and then was pressed onto the nickel foil (25 MPa), which served as a current collector (surface was 0.785 cm2 ). The typical mass weight of electrode material was 30 mg. The used electrolyte was 2 M KCl. 2.2. Characterization The electrochemical measurements were performed using an Autolab (Netherlands) potentiostat Model PGSTAT 302N. CV tests were conducted at various scan rates (s) with recording of potential response currents, I, which is related by C¼I/s where C is the capacitance of the electrode interface. The specific capacitance C (FgÀ1 ) of the active material was determined by integrating either the oxidative or reductive parts of the cyclic voltammogram curve to obtain voltammetric charge Q (C). This charge was divided by mass of active material m (g) in the electrode and width of the potential window of the cyclic voltam- mogram ΔE (V), i.e., C¼Q/(ΔEm) [7]. The morphology and nature of the prepared electrodes were studied using scanning electron microscopy (TESCAN, USA). 3. Results and discussion Nanoparticles distribution quality on the electrode surface is one of the key parameters which controls the electrical performance of nanoparticle containing electro- des for supercapacitors. Using macroparticles like used carbon black particles which store electrical energy through the double layer mechanism, will make macro- pores and macrogrooves with deep and hollow shapes on surface of the electrode. Using the nanoparticles will make nanopores with shallow shapes. Therefore, mixing the nanoparticles with macroparticles will have a significant effect on the morphology and nature of the prepared electrodes. One of the thinkable morphology changes by mixing of the nanoparticles with macroparticles is schematically illustrated in Fig. 1. In the absence of the nanoparticles, macrogrooves produced between CB parti- cles and these grooves are exposed to the electrolyte for charge storage (Fig. 1(a)). As the nanoparticle content of Fig. 1. (a–d) Schematic illustration of the surface changes by addition of nanoparticles into the electrode material and, (e) SEM image obtained from 30:60:10 electrode. (For interpretation of the references to color in this figure, the reader is referred to the web version of this article.) Fig. 2. Nyquist diagrams of different ZrO2-content electrodes in 2 M KCl electrolyte. M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264 261
  • 3. the electrodes increases the macropores are filled with nanoparticles and the depth of the macrogrooves are decreased (Fig. 1(b) and (c)). Then, all grooves are filled and the CB particles on the surface of the electrode are covered with a thin layer of ZrO2 nanoparticles and finally, macrogrooves are replaced with the nanoporous structure prepared by the nanoparticles (Fig. 1(d)). Therefore, active surface used for charge storage on the surface of the electrode is replaced and this increases the specific surface area of the prepared electrodes. SEM images obtained from 30:60:10 (CB:ZrO2:PTFE) electrodes (Fig. 1(e)) confirm the presence of macrogrooves made between the CB particles (were shown by red lines) which nearly filled with ZrO2 nanoparticles. In these electrodes, CB particles can provide a conductive channel due to their excellent conductivity. Unlike the CB particles, metal oxides like ZrO2 are low conductive materials but, have a pseudo capacitive char- acteristic which can take place in redox reactions and improve the energy storage capability of the electrodes. This low conductivity decreases the charge stored on the electrodes, especially at high sweep rates. Therefore, as the nanoparticle content of the electrode increases, it is proposed that the total charge stored on the electrode surface increases, at first, due to increasing the specific surface area and changing the charge storage mechanism from double layer to pseudo, and then decreases due to increasing the electrical resistance of the electrode. The principle reaction involved in the charging and discharging processes of zirconium dioxide in an aqueous electrolyte can be described by reaction (1) ZrIV O2 þλþ þeÀ 2ZrIII OOλ ð1Þ where λ denotes Kþ , Hþ . Additionally, two mechanisms can be proposed for supercapacitive charge storage in ZrO2. The first mechan- ism is based on the intercalation/extraction of protons or Fig. 3. Capacitance vs. potential curves obtained from (a) 90:00:10, (b) 50:40:10, (c) 30:60:10, (d) 20:70:10 and (e) 10:80:10 electrodes in 2 M KCl electrolyte. M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264262
  • 4. alkali cations into the oxide particles (denoted as reaction (2)), whereas the second mechanism involves the surface adsorption/desorption of proton or alkali cations probably (denoted as reaction (3)): ZrO2 þMþ þeÀ ¼ ZrOOM ð2Þ and ðZrO2Þsurface þMþ þeÀ ¼ ðZrOOMÞsurface ð3Þ where Mþ denotes Kþ or H3Oþ . In order to gain a quantitative information on the effect of surface changes on charge storage mechanism of the ZrO2/CB electrodes by increasing the nanoparticle content of the electrodes, the voltammograms obtained from different nanoparticle containing electrodes were analyzed as a func- tion of scan rate, according to the procedure reported by Ardizzone et al. [8]. Then, the total charge and charge related to the most accessible surface area were calculated. Four prominent characteristics can be reported by chan- ging the nanoparticle content of the electrodes from obtained CV curves (Fig. 3): changing the shape of the CV curves, changing the specific capacitance, deviation of the CV curves from the classical square waveform expected for a pure capacitor by increasing the sweep rate and, increasing the voltage reversal at end potentials. As the nanoparticle content of the electrodes increases electrical resistance of the electrode increases (Fig. 2) and, up to 60%, the energy stored on the electrode increases at first and then decreases due to the electrical resistance and specific surface area changes of the electrodes. Additionally, scan rate dependence of the capacitance can be related to the less accessible surface area (pores, cracks, etc) which become excluded as the rate reaction is enhanced [9,10]. Ion diffusion ability of the electrolyte into the surface of the electrode will have a significant effect on the voltage reversal of the electrodes. Improvement of the voltage reversal of the high nanoparticle containing electrodes may be related to surface morphology changes which change the active energy storage sites from down the deep macropores to shallow nanopores. Calculat- ing the total charge stored on electrodes and the charge stored on less and more accessible surface area of the electrodes are efficient indicators which indicate the charge distribution on the electrode. In charge and discharge cycles, the total charge can be written as a sum of an inner charge from the less accessible reaction sites and an outer charge from the more accessible reaction sites, i.e., q* T¼q* I þq* O, where q* T, q* I and q* O are the total charge and charges related to the inner and the outer surfaces, respectively [11]. The extrapolation of q* to v¼0 from 1/q* vs. v1/2 plots obtained from different nanoparticle containing electrodes (Fig. 4(a)) give the total charge qT which is the charge related to the entire active surface of the electrode. In addition, extrapola- tion of q* to v¼1 (vÀ1/2 ¼0) from the q* vs. vÀ1/2 plots (Fig. 4(b)) give the outer charge q* O, which is the charge due to redox process on the most accessible active surface [8,11]. Total and outer charges vs. nanoparticle content of the electrode obtained from different nanoparticle electrodes were plotted in Fig. 4(c). Total and outer charge plots confirm that the addition of nanoparticles increases and then decreases the charge stored on the electrode surface, as expected and explained above. Although, electrodes which contain higher nanoparticle contents show higher ratio of the outer charge to total charge (q* O/q* T) (increases from 0.05 to 0.18) which confirms the higher current response on voltage reversal of high nanoparticle containing electrodes. Finally, it is concluded that the 40:50:10 (CB:ZrO2:PTFE) electrodes show better charge storage capability ($57C gÀ1 cmÀ2 ) (Fig. 4(c)). It may be due to the synergistic effect of the double layer characteristic of the CB particles and the pseudo characteristic of the ZrO2 nanoparticles. Changing the surface morphology from macrogrooves to nanoporous structure makes the 10:80:10 electrode to show the high outer charge to total charge (q* O/q* T) ratio of as-high-as 0.18 which confirms its high current response on voltage reversal. 4. Conclusions In this study, effect of nanoparticle content of the ZrO2/ carbon black nanocomposite electrodes on the microstruc- ture, nature and the electrochemical performance of the prepared electrode were investigated. SEM images confirm Fig. 4. (a) Extrapolation of q to v¼0 from the qÀ1 vs. v0.5 plot given the total charge and (b) extrapolation of q to v¼1 from the q vs. vÀ0.5 plot given the outer charge for CB electrodes. (c) Total and outer charge stored on the different nanoparticle containing electrodes. M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264 263
  • 5. the surface changes from hallow macrogrooves to shallow nanoporous structure by increasing the nanoparticle content of the electrodes. Charge stored on the electrode surface increases ($57C gÀ1 cmÀ2 obtained from 40:50:10 elec- trode) at first, due to the synergistic effect of the carbon black and ZrO2 nanoparticles, and then decreases by increas- ing the nanoparticle content due to the electrical resistance of the electrode. Finally, it is concluded that the current response of the electrodes (q* O/q* T ratio of 0.18 obtained from 10:80:10 electrode) increases by addition of the nanoparti- cles due to the surface changes from hollow macrogrooves to the nanoporous structure. References [1] W. Wei, X. Cu, W. Chen, D.G. Ivey, J. Power Sources 186 (2009) 543–550. [2] R. Kotz, M. Carlen, Electrochim. Acta 45 (2000) 2483–2498. [3] I. Hadjipaschalis, A. Poullikkas, V. Efthimiou, Renew. Sustain. Energy Rev. 13 (2009) 1513–1522. [4] Y. Zhang, H. Feng, X. Wu, L. Wang, A. Zhang, T. Xia, Int. J. Hydrog. Energy 34 (2009) 4889–4899. [5] B.E. Conway, Electrochemical Capacitors Scientific Fundamental and Technological Applications, Klumer Academic/Plenum, New York, 1999, 105–124. [6] B. Babakhani, D.G. Ivey, J. Power Sources 195 (2010) 2110–2117. [7] G. Sun, W. Song, X. Liu, W. Qiao, D. Long, L. Ling, Mater. Lett. 65 (2011) 1392–1395. [8] S. Ardizzone, G. Fregonara, S. Trasatti, Electrochim. Acta 35 (1990) 263–267. [9] B.E. Conway, W.G. Pell, J. Power Sources 105 (2002) 169–181. [10] M. Nasibi, M.A. Golozar, Gh. Rashed, Mater. Lett. 91 (2013) 323–325. [11] M. Nasibi, M.A. Golozar, Gh. Rashed, Mater. Lett. 85 (2012) 40–43. M. Nasibi et al. / Materials Science in Semiconductor Processing 24 (2014) 260–264264