Accepted Manuscript Impact of nanofluidic electrolyte on the energy storage capacity in vanadium redox flow battery
Jungmyung Kim, Heesung Park PII:
S0360-5442(18)31286-6
DOI:
10.1016/j.energy.2018.06.221
Reference:
EGY 13263
To appear in:
Energy
Received Date:
20 March 2018
Accepted Date:
29 June 2018
Please cite this article as: Jungmyung Kim, Heesung Park, Impact of nanofluidic electrolyte on the energy storage capacity in vanadium redox flow battery, Energy (2018), doi: 10.1016/j.energy. 2018.06.221
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ACCEPTED MANUSCRIPT
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Impact of nanofluidic electrolyte on the energy storage capacity in vanadium redox flow battery
2 3 4
Jungmyung Kim, Heesung Park*
5
Department of Mechanical Engineering, Changwon National University
6 7
Abstract
8
The limitation of energy storage capacity in vanadium redox flow battery impedes further
9
commercialization of the battery. The concept proposed in this study is to overcome the limit
10
by using nanofluidic electrolytes. Multi-walled carbon nanotubes (MWCNTs) are chosen to
11
disperse in electrolytes due to their high surfaces to volume ratio. Nanofluid electrolytes with
12
three electrolyte weight percent MWCNT (0.05, 0.1, 0.2 wt%) were tested and compared with
13
the pristine electrolyte. Half-cell test with cyclic voltammetry has shown that electrochemical
14
reaction performance is proportional to the content of MWCNT in nanofluidic electrolytes. The
15
redox reaction of nanofluidic electrolytes are enhanced by the increased electrochemical
16
activity and reversibility in addition to the lower polarization effect. Meanwhile, single-cell
17
test reveals that the optimum weight percent of nanofluidic electrolytes is 0.1% of MWCNT
18
because the electrolyte containing 0.2% of MWCNT induces the unwanted precipitation at the
19
electrodes during the electrochemical reaction. After completion of 62 charge/discharge
20
cyclings, nanofluidic electrolyte with 0.1% MWCNT retains specific discharge capacity of
21
31.7 Ah L-1 while pristine electrolyte does 26.0 Ah L-1. This corresponds to 22% enhancement
22
of energy storage by using the nanofluidic electrolytes. We conclude that nanofluidic
23
electrolytes can considerably improve the energy storage capacity with optimized content of
24
MWCNT.
25 26 27
Keywords: Active area, Electrochemical performance, Energy storage capacity, Nanofluidic electrolyte, Vanadium redox flow battery
28 29 30 31 32
Corresponding author Mechanical Engineering Department of Changwon National University, 20 Changwondaehak-ro, Changwon City, 51140 South Korea Telephone: +82-55-213-3609 1
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Email address:
[email protected]
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1. Introduction
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The current energy supply policy is facing a problem of inconsistency of power
36
demand/supply and limited conditions of large-scale power utility [1,2]. The energy storage
37
system is a promising technology to tackle the problem by compromising the power demand
38
and supply [3]. Vanadium redox flow battery (VRFB) is a strong candidate for the energy
39
storage system (ESS) application due to the benefits of extensibility, independent capacitance,
40
high energy efficiency, long lifetime, and free from cross-over contamination [4-6]. Various
41
redox couples [7], cell components [8,9], and optimum operating conditions [10,11] have been
42
under investigation to increase electrochemical performance and optimum efficiency.
43
Although the energy storage of VRFB extends to 4–40 MW for the distributed and smart grid
44
applications [12], there still requires a breakthrough technology to overcome low energy
45
storage density of VRFB. Zhang et al. have shown that the discharge capacity of VRFB was
46
enhanced by effectively mixing the electrolyte [13]. Nonetheless, lithium-ion battery offers up
47
to 500 Wh L-1 whereas VRFB does 33 Wh L-1 due to the limited solubility of vanadium species
48
(1-2 M) [14,15]. Therefore, a progressive technology is required to overcome the limitation of
49
energy storage density in VRFB.
50
On the other hand, novel approaches to energy efficiency and capacity enhancement have
51
been investigated, most of which have demonstrated increased electrochemical properties
52
using nano-sized materials. Especially, nanoparticles have drawn attention to increase
53
electrochemically active sites of carbon felt electrode in VRFBs. Bismuth nanoparticles [16]
54
and niodium oxide nanorods [17] were employed to replace noble metal with offering high-
55
performance electrodes for VRFBs. Li et al. [18] demonstrated that single-walled carbon
56
nanotubes served an electrode catalyst for VRFBs. Wu et al. proposed cost effective and a high-
57
performance electrode by growing N-doped carbon nano-spheres on graphite felt fibres [19].
58
They demonstrated the superior performances of energy efficiency and capacity retention by
59
conducting single cell test. Li et al. investigated carbon electrode with hollow nanofibers which
60
provided more active sites, higher pore volume, and short diffusion pathways for ions and
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electrons resulting in enhanced energy storage [20]. Blasi et al. achieved high electrochemical
62
performance in VRFB by using the electrode based on carbon nanofiber with Mn3O4
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nanoparticles [21]. Meanwhile, nanofluids have been also used to improve thermal properties,
64
lubrication and combustion characteristics [22-24]. There have been a few attempts [15,25] to
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develop electroactive nanofluids for VRFB; however, significant changes are inevitable to
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apply nano-sized material technology to the already commercialized VRFB energy storage 3
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devices. The motivation of our study is to economically and effectively increase
68
electrochemical performance and energy storage capacity by dispersing nano-sized materials
69
in electrolytes used in existing installations. In this regard, nanofluidic electrolyte is
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manufactured by using multi-walled carbon nanotubes (MWCNT). The liquid produced in the
71
laboratory is a colloidal suspension of MWCNT solid nanoparticles in aqueous electrolyte. We
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have chosen MWCNTs as nanoparticles due to their high porosity and surface-to-volume ratio,
73
which offers increased electroactive sites resulting in the enhanced electrochemical kinetics of
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VRFB. The electrochemical performance has been compared between pristine (zero MWCNT)
75
and nanofluidic electrolytes with different MWCNT concentrations. It is shown that the
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MWCNT nanofluidic electrolytes significantly increase reversibility and active area at the
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reaction zone. After conducting 62 cycling test by using single cell, nanofluidic electrolyte with
78
0.1 weight percent (wt%) MWCNT is found to retain specific discharge capacity of 31.7 Ah
79
L-1 which is 22% higher than pristine electrolyte.
80 81 82
2. Experimental 2.1 Characterization of materials
83
The nanostructures of MWCNTs were analyzed by field emission transmission electron
84
microscopy (TEM, JEM 2100F, JEOL) and X-ray diffractometer (D8 Discover, BRUKER)
85
operated at 160-200 kV and 40 kV, respectively. Raman spectroscope (JP/NRS-3300, JASCO)
86
equipped with a 100 mW solid-state primary laser at 532 and 785 nm was used to identify the
87
compositions of the materials. The surface morphologies of carbon felt electrodes were
88
inspected by using a field emission scanning electron microscope (SEM, Merlin compact,
89
ZEISS) operating at 5 kV. Optical microscope (JP-E600, Nikon) was also used to visualize the
90
dispersion of MWCNTs in nanofluidic electrolytes.
91 92
2.2 Preparation of nanofluidic electrolytes
93
The pristine electrolyte used in the experiments was prepared by electrochemical
94
decomposition of 1.6 M VOSO4 and 4 M H2SO4 solution [26]. The positive and negative
95
electrolytes were divided into electrolytes of different valence states (V3+/VO2+) after
96
conducting 40 mA cm-2 constant current on 10 charge/discharge cycles. With these electrolytes,
97
different wt% MWCNT nanofluidic electrolyte were produced to secure experimental
98
consistency. Graphene has a hexagonal carbon ring bond of carbon atoms in a two-dimensional
99
plane, and when it is connected in the form of a hollow cylinder, it becomes a carbon nanotube. 4
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There are two types of carbon nanotubes depending on their shape. Having a cylindrical single-
101
layer graphene is Single-walled Carbon nanotube (SWCNT). MWCNT has about 50-cylinder
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graphene layers [22]. The MWCNTs of outer diameter in the range of 30–50 nm (40-45 walls)
103
with length ranging from 10 to 20 μm were supplied by Carbon Nanotubes Plus, USA, with
104
specifications as listed in Table 1. Fig. 1a and b show the TEM and SEM images of a single
105
MWCNT and MWCNT powder, respectively. The multiple graphitic edge planes of MWCNTs
106
can be observed in the image. As shown in Fig. 1c and d, three different weights of MWCNT
107
powders were homogeneously dispersed by the 490 W sonicator in the pristine electrolytes for
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comprising 0.05, 0.1 and 0.2 wt% nanofluidic electrolytes, respectively. It should be denoted
109
that the temperature of sonicator was kept at 23 ± 1 °C to prevent unwanted precipitation of
110
the electrolyte as illustrated in Fig. 1e. The dispersion of nanofluidic electrolytes was visually
111
inspected by optical microscopy as displayed in Fig. 1f. It can be seen that the MWCNTs were
112
homogeneously dispersed for all nanofluidic electrolytes.
113
114 115
Fig. 1. Schematic diagram of manufacturing process of nanofluidic electrolytes; (a) TEM (b)
116
SEM images; (c) predefined amounts of MWCNTs; (d) positive and negative electrolytes; (e) 5
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temperature controlled sonicator; (f) dispersed MWCNTs images by taking sample nanofluidic
118
electrolytes after completion of dispersing process.
119 120
Table 1 Details information of multi-walled carbon nanotubes. Item Manufacturer Product number Average particle size Surface area (SSA) Purity Tap density Aspect ratio Electrolytic conductivity
121
Specification Carbon Nanotubes Plus, USA GCM335 30-50 nm diameter, 10-20 μm length >100 m2 /g >98 wt% 0.22 g/cm3 333-400 >100 s/cm
122
2.3 Half-cell test
123 124
The electrochemical properties of the pristine and nanofluidic electrolytes were measured
125
by using cyclic voltammetry (CV, NuVant System, Powerstat-05) test with three electrodes.
126
Electric potential variations were recorded by using a saturated silver-silver chloride double-
127
junction cell as a reference electrode, while the counter and working electrodes were a spiral
128
platinum (Ag/AgCl) and glassy carbon (7.065 mm2), respectively. The volume of electrolyte
129
used in the test was 15 mL for all cases. The applied scan rate was varied from 5 to 200 mV s-
130
1
131
the current density was measured for 50 cycles with the scan rate of 20 mV s-1.
to investigate the energy storage capacity of the nanofluidic electrolytes. For CV cycle test,
132 133
2.4 Single cell test
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The VRFB single cell with 25 cm2 of active area was composed of polytetrafluoroethylene
135
gaskets, bipolar plates (BLUE 100-BP, Standard Energy), 4.6 mm thickness carbon felt
136
electrodes (SIGRACELL, GFD 4.6 EA, SGL) in thickness of 3 mm after compression, a Nafion
137
membrane (NR-117) and an oxygen-free copper current collecting plates as illustrated in Fig.
138
2 [26]. In order to improve the electrical conductivity, corrosion resistance and brittleness of
139
copper, oxygen-free copper prepared so that the oxygen content is 0.008% or less through
140
deoxidizing agent was used. The cell was connected with a power supply (Sorensen HPD series,
141
AMETEK) and an electronic load (PLZ164W, KIKUSUI) for conducting charge/discharge 6
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cycle test. The electrolyte flow rate was defined to 50 mL min-1 with the volume of electrolyte
143
of 50 mL, while the cell potential was limited between 1.7 V and 0.8 V for charge and discharge,
144
respectively. A specially designed pneumatic fixture applied the constant compression force of
145
0.5 MPa between two endplates. With this, it was confirmed that the sealing of the single cell
146
including fitting parts was secured by preventing unwanted leak of electrolytes. During
147
experiment, purge gas (N2) was supplied to each bottle to eliminate air intrusion. The
148
experiments of charge/discharge cycles were conducted by applying constant electrical current
149
of 120 mA cm-2. After the completion of experiments, the used carbon electrodes were taken
150
and analyzed by SEM.
151
(a)
(b)
PTFE housing
Bipolar plate Membrane
Outlet
Current collector
Inlet
Active area Inlet Outlet
152 153
Fig. 2. (a) Schematic diagram of 25 cm2 single cell. (b) Schematic illustration of MWCNT
154
nanofluidic electrolytes in the active area.
155 156 157
3. Results and discussion 3.1. Physico-chemical analysis
158
The X-ray diffraction patterns of MWCNT and carbon felt electrode are depicted in Fig. 3a.
159
It can be seen that the peak intensities of 2θ = 25.6 ° and 2θ = 23.9 ° reflect the graphite
160
composition of (002) and (100), respectively. Fig. 3b compares the Raman spectra of MWCNT
161
and carbon felt electrode. The D bands (first peak) of the two materials were commonly
162
presented at 1340 cm-1. Since the D band reflected the content of graphitic edge which became
163
the active sites (defects) of the graphite materials [15], it could be expected that the presented
164
D band in MWCNT increased the active sites during the electrochemical reaction in VRFB.
165
Furthermore, the G band (second peak) commonly was found at 1580 cm-1. The intensity ratio
166
of the D band to the G band is an indicator of the amount of defect present in the carbon 7
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materials [27]. It can be seen that the carbon felt electrode had more active sites than the
168
MWCNT.
169
The rheological behavior of the nanofluidic electrolytes at different wt% MWCNT was
170
studied by using glass-capillary viscometer. The measured viscosity was 4.455, 4.785, 5.081
171
and 7.481 mPa s for pristine, 0.05, 0.1 and 0.2 wt% electrolyte, respectively. The increment of
172
viscosity by nanofluidic electrolyte was 7.4 and 14.1 % for 0.05 and 0.1 wt% MWCNT,
173
respectively while it was 68.1 % for 0.2 wt% MWCNT. The viscosities in the range of 4.4 –
174
5.08 mPa s were very close to that measured by Li et al. [28]. Nonetheless, significant increase
175
of viscosity for 0.2 wt% MWCNT might be inappropriate in the practical application.
176 G band
D band
177 178
Fig. 3. (a) X-ray diffraction patterns and (b) Raman spectra of MWCNTs and carbon felt.
179 180
3.2. Electrochemical behavior of nanofluidic electrolyte
181
To investigate the effect of nanofluidic electrolyte on the electrochemical reaction, CV tests
182
were performed for positive (VO2+/VO2+) and negative (V2+/V3+) electrolytes with 0 (pristine),
183
0.05, 0.1, and 0.2 wt% MWCNT, respectively. Fig. 4a and b show the oxidation-reduction CV
184
curves when the scan rate was 5 mV s-1 for the positive and negative electrolytes. It should be
185
denoted that the potential window was defined to 0.2-1.6 V (positive electrolyte) and -1.2-0.4
186
V (negative electrolyte). For both of the positive and negative electrolyte, the measured
187
oxidation-reduction peak current densities were in the order of MWCNT content. The increased
188
peak current density was caused by the improved electron transfer kinetics of VO2+/VO2+ and
189
V2+/V3+ couples [29]. Therefore, it can be seen that the electrochemical activities of the positive 8
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and negative nanofluidic electrolyte were enhanced by increasing MWCNT content. This
191
increase in activity is due to the graphitic region of the MWCNT, which can increase the active
192
area and the active interface provided by conventional electrodes. The increased active sites of
193
nanofluidic electrolyte also improved the oxidation potential from 1.066 V (0 wt%) to 1.028 V
194
(0.05, 0.1, 0.2 wt%). The nanofluidic electrolyte with 0.2 wt% MWCNT exhibited the good
195
electrochemical performance considering large peak current density and small oxidation-
196
reduction potential difference. Furthermore, the peak current density variations with respect to
197
different nanofluidic electrolytes and scan rates are presented in Fig. 4c and d. The peak current
198
density was linearly proportional to the square root of the scan rate by using Randles-Sevcik
199
equation, indicating that the electrochemical reaction at each electrode was controlled by
200
diffusive mass transfer at double-layer [30]. It is clearly observed that the slope of the curve
201
increased with the MWCNT content of the nanofluidic electrolyte due to accelerated mass
202
transfer rate. In this, the nanoparticles in the nanofluidic electrolyte enhanced the
203
electrochemical performance through a double layer mechanism.
204
The peak current densities (Ipox and Ipre, for oxidation and reduction, respectively), ratios of
205
peak current density (Ipox/Ipre) and oxidation-reduction peak potential differences (ΔEp) are
206
summarized in Table 2. Although peak current density increased with MWCNT content in
207
electrolyte, the minimum ratio of peak current density and peak potential difference were 1.38
208
and 0.14 V for 0.1 wt% positive nanofluidic electrolyte. Nonetheless, minimum peak potential
209
difference was presented when 0.05 wt% MWCNT negative nanofluidic electrolyte was used.
210
The impact of nanofluidic electrolyte on the electrochemical reaction could be seen by the
211
experiment; however, the optimal wt% of MWCNT was still unclear. In this regard, CV cycle
212
test was also carried out to further investigate the effect of MWCNT content in electrolyte on
213
the long-term stability.
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30
(b)
20
-2
Current density (mA cm )
-2
Current density (mA cm )
(a) 10 0 -10 -20
Pristine 0.05 wt% 0.1 wt% 0.2 wt%
VO2+ VO2 + Reduction
-30 0.2
0.4
0.6
0.8
1.0
1.2
1.4
Voltage (V vs. Ag/AgCl)
160 -2
120
Peak current density (mA cm )
-2
Peak current density (mA cm )
214
0 -10 Pristine 0.05 wt% 0.1 wt% 0.2 wt%
-20
-1.0
-0.8
-0.6
-0.4
6
8
-0.2
0.0
0.2
0.4
10
12
14
16
Voltage (V vs. Ag/AgCl)
80
(c)
140 100 80 60
Pristine 0.05 wt% 0.1 wt% 0.2 wt%
40 20 0 -20 -40 -60 -80 -100
10
-30 -1.2
1.6
Oxidation V2+ V3+
20
0
2
4
6
8
1/2
(Scan rate)
10
-1 1/2
12
14
16
(d)
60 40 20 0 -20 -40
Pristine 0.05 wt% 0.1 wt% 0.2 wt%
-60 -80 -100
0
2
4
1/2
(Scan rate)
(V s )
-1 1/2
(V s )
215
Fig. 4. Cycle voltammograms of the tested electrolytes: (a) positive electrolyte, (b) negative
216
electrolyte at a scan rate of 5 mV s-1. Plot of the peak current density according to Randles-
217
Sevcik equation for (c) positive and (d) negative electrolytes, respectively.
218 219
220
Table 2 Summary of cyclic voltammetry results for the pristine and nanofluidic electrolytes. Sample Ip ox (mA cm-2 ) Positive electrolyte Pristine 19.6 0.05 wt% 27.8 0.1 wt% 31.0 0.2 wt% 32.1 Negative electrolyte Pristine 3.08 0.05 wt% 6.09 0.1 wt% 6.69 0.2 wt% 9.19
Ip re (mA cm-2 )
Ip ox /Ip re
ΔEp (V)
-13.7 -19.9 -22.4 -22.5
1.43 1.40 1.38 1.43
0.22 0.14 0.14 0.14
-9.73 -16.7 -15.9 -24.0
0.32 0.36 0.42 0.38
1.04 0.89 0.89 0.96
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The electrochemical stability of the nanofluidic electrolytes were investigated by conducting
223
50 charge/discharge cycling test. Fig. 5a shows that the peak current densities of positive
224
pristine electrolyte were considerably reduced for oxidation-reduction reaction after 50
225
charge/discharge cycles, whereas nanofluidic electrolytes with 0.1 and 0.2 wt% MWCNT
226
showed unchanged peak current densities during the cycles. Meanwhile, negative pristine and
227
0.2 wt% nanofluidic electrolytes indicated clear reductions of peak current densities after 50
228
cycles as depicted in Fig. 5b. In this regard, the peak current densities corresponding to the
229
cycle number are displayed in Fig. 5c and d for oxidation reaction. It can be found that the
230
reduction ratios of peak current density were 19.8% (pristine), 6.84% (0.05 wt%), 1.11% (0.1
231
wt%), and 1.61% (0.2 wt%) for positive electrolytes, while the ratios were 50.4% (pristine),
232
12.9% (0.05 wt%), 6.73% (0.1 wt%), and 37.3% (0.2 wt%) for negative electrolytes. The
233
irreversible electrochemical reaction reduced electrochemical activity and peak current density
234
during the cycles. Meanwhile, the MWCNT dispersed in nanofluidic electrolyte retained the
235
activity through the double layer mechanism at the graphitic region of MWCNTs. It is evident
236
that the nanofluidic electrolytes offered more stable electrochemical reaction after 50
237
charge/discharge cycles than pristine electrolyte. The MWCNTs dispersed in electrolyte
238
contributed to increase active sites (see Fig. 3b) resulting in high stable electrochemical
239
reaction. It is also denoted that the positive and negative nanofluidic electrolyte with 0.1 wt%
240
MWCNT showed almost unchanged peak current densities during the cycles indicating
241
minimum irreversible loss.
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60
30
30 20 10
20 -2
Current density (mA cm )
40
-2
Current density (mA cm )
50
(b)
(a)
st
Pristine 1 Cycle th Pristine 50 Cycle st 0.05 wt% 1 Cycle th 0.05 wt% 50 Cycle st 0.1 wt% 1 Cycle th 0.1 wt% 50 Cycle st 0.2 wt% 1 Cycle th 0.2 wt% 50 Cycle
0 -10 -20 -30 0.4
0.8
1.2
Voltage (V vs. Ag/AgCl)
st
Pristine 1 Cycle th Pristine 50 Cycle st 0.05 wt% 1 Cycle th 0.05 wt% 50 Cycle st 0.1 wt% 1 Cycle th 0.1 wt% 50 Cycle st 0.2 wt% 1 Cycle th 0.2 wt% 50 Cycle
-10 -20 -30
-1.2
-0.9
-0.6
-0.3
0.0
0.3
0.6
Voltage (V vs. Ag/AgCl) -2
(c) 55 50 45 40
30 Pristine 0.05 wt% 0.1 wt% 0.2 wt%
25
(d)
20 15 10 5
2+
3+
Pristine 0.05 wt% 0.1 wt% 0.2 wt%
35
0
-40 -1.5
1.6
V V peak current density (mA cm )
2+
242
0.0
60
+
-2
VO VO2 peak current density (mA cm )
-40 -0.4
10
30
0
10
20
30
40
50
Cycle number
0
0
10
20
30
40
50
Cycle number
243
Fig. 5. CV curves of (a) positive electrolytes, and (b) negative electrolytes at the scan rate of
244
20 mV s-1; peak current density variations of (c) positive and (d) negative during oxidation
245
reaction against cycle number.
246 247
3.4. VRFB single cell performance
248
The performance evaluation of VRFB single cell is significant to characterize the effect of
249
nanofluidic electrolyte on the porous electrode. Four different positive and negative
250
electrolytes which contained pristine, 0.05, 0.1 and 0.2 wt% MWCNT were prepared. To
251
prevent contamination between the sample electrolytes, the components of single cell were
252
replaced for each experiment. VRFB single cell performance was evaluated by conducting 62
253
charge/discharge cycles test with a constant current of 120 mA cm-2. The energy storage
254
capacity was evaluated by multiplying the applied current and time at cut-off voltage (0.8 V)
255
for the reservoir volume of electrolyte. Fig. 6a and b display the voltage variations for the
256
nanofluidic electrolytes at first and sixty-second cycles. Comparing Fig. 6a and b, the capacity 12
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retention of the pristine electrolyte was 84.5% after 62 cycles, but the nanofluidic electrolytes
258
showed 90.1, 92.6, and 88.8% capacity changes, respectively. The retention of energy storage
259
capacities was improved when the nanofluidic electrolytes were used. It can be seen that the
260
nanofluidic electrolyte increased the VRFB single cell performance and energy storage
261
capacity during the charge/discharge cycles. This corresponds to the reduced potential
262
difference (decreased polarization effect) as listed in Table 2.
263 1.7
1.7
1.6
1.6 2.0
1.2 1.1
1.0
1.0
1.5
1.3 1.2 1.1
1.0
1.0
(a)
0.9 0.8
Pristine 0.05 wt% 0.1 wt% 0.2 wt%
1.4
B
Cell voltage (V)
1.5
1.3
2.0
1.5
Pristine 0.05 wt% 0.1 wt% 0.2 wt%
1.4
B
Cell voltage (V)
1.5
0
0.5
5
10
15
0.0
20
25
30
0.8
35
0
5
-1
Specific capacity (Ah L )
264
(b)
0.9
0.0
0.5
1.0
0.5
10
15
20
25
0.0
Specific capacity (Ah L )
1.5
2.0
30
35
-1
0.0
0.5
A
A
265
Fig. 6. Voltage variations during charge/discharge cycling test at 120 mA cm-2; (a) 1st cycle,
266
(b) 62nd cycle.
35
42.0
34
40.7
33
39.4
32
38.1
31
36.8
30
35.5 34.2
29 Pristine 0.05 wt% 0.1 wt% 0.2 wt%
27 26 25
0
10
20
32.9 31.6
Energy density (Wh L-1)
Specific discharge capacity (Ah L-1)
267
28
30.3
30
40
50
60
29.0
268
Cycle number
269
Fig. 7. The variations of specific discharge capacity during the single cell cycle test for the
270
pristine and nanofluidic electrolytes. 13
1.0
1.5
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To further investigate electrochemical performance during the cycling test, the variations of
272
the specific discharge capacity and energy density against cycle number are illustrated in Fig.
273
7. There can be seen the significant increase in the specific discharge capacity for nanofluidic
274
electrolytes at the beginning of the cycle test. In addition, the retentions of specific discharge
275
capacity during cycling test were 87, 94, 101 and 90% for pristine, 0.05, 0.1, and 0.2 wt%
276
electrolytes, respectively. This indicates the superior long-term stability of the nanofluidic
277
electrolytes in accordance with CV test depicted in Fig. 5. It is noted that the 0.1 wt%
278
nanofluidic electrolyte retained 22% more specific discharge capacity than pristine electrolyte
279
after 62 cycles. For the pristine electrolyte, the small increase of the capacity (3.3 % of initial
280
value) until 25th cycle was caused by imbalance of vanadium valence states or electrolyte
281
volume change [31]. In this, the capacity at 25th cycle was 30.4, 30.5, 34.1 and 32 AhL-1 for
282
pristine, 0.05, 0.1, and 0.2 wt% electrolyte, respectively. The capacity decay rate from 25th to
283
62nd cycle was 0.4, 0.18, 0.18 and 0.3 % per cycle for the same order of MWCNT concentration
284
electrolyte. It can be found that 0.1 wt% electrolyte produced highest capacity and capacity
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retention.
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Meanwhile, the significant fluctuation of capacity during the cycles for 0.2 wt% electrolyte
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was detected in Fig. 7. In this regard, carbon felt electrodes were sampled after completion of
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each experiment to investigate the surface morphology. Fig. 8 shows the observed images taken
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by SEM for the pristine and nanofluidic electrolyte. In particular, considerable coagulations of
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electrolyte were observed in Fig. 8g and h (0.2 wt% nanofluidic electrolyte), which was enough
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to impede electrolyte flow as well as decrease active area of the porous electrode. This is the
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reason why the nanofluidic electrolyte with 0.2 wt% MWCNT presented the significant
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fluctuation capacity and lower electrochemical performance during the cycle test than the
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nanofluidic electrolyte with 0.1 wt% MWCNT as shown in Fig. 7. In this, 0.1 wt% nanofluidic
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electrolyte was optimum to enhance energy storage capacity with stable electrochemical
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reaction in VRFB. In this experimental analysis, the electrical double layer established at each
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nanoparticle increased the energy storage capacity. Although MWCNT concentration of 0.1 wt%
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was used, however, the stored energy at each particle due to electrical double layer was
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transferred to the porous electrode by diffusion and convection. Consequently, there were two
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different mechanisms. One is the electron pathway established between electrolyte and
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electrode interface. The other is direct transportation of each nanoparticles to electrode.
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Nonetheless, 0.2 wt% MWCNT increased viscosity up to 68.1 % than pristine electrolyte and
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induced large amount of precipitation at the porous electrode. 14
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304 (a)
10μm
(e)
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(b)
10μm
10μm
(g)
(f)
10μm
(c)
10μm
10μm
(d)
10μm
(h)
10μm
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Fig. 8. SEM images of carbon felts after completion of single cell test; (a, b) pristine electrolyte;
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(c, d) 0.05 wt% MWCNT electrolyte; (e, f) 0.1 wt% MWCNT electrolyte; (g, h) 0.2 wt%
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MWCNT electrolyte.
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4. Conclusions
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In this study, the experimental results were introduced to present the feasibility of nanofluidic
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electrolyte in VRFB. The MWCNTs were chosen as the nanoparticles to manufacture
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nanofluidic electrolyte. The physio-chemical analysis of the MWCNTs revealed the increased
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active sites of the electrochemical reaction. CV test was carried out to investigate the
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electrochemical reaction kinetics of V2+/V3+ and VO2+/VO2+ vanadium redox couples by using
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nanofluidic electrolytes. The measured peak current densities and electric potential differences
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indicated the improved reversibility and polarization effect resulting in enhanced
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electrochemical performance in the order of MWCNT content. In addition, it is evident that the
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nanofluidic electrolytes offered more stable electrochemical reaction after 50 charge/discharge
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cycles than pristine electrolyte. The optimum weight percent of MWCNT in electrolyte was
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revealed to 0.1 wt% by conducting VRFB single cell test whereas 0.2 wt% nanofluidic
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electrolyte induced large amount of precipitation which impeded the electrolyte flow and
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decreased active sites resulting in low electrochemical performance and energy storage
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capacity. Comparing with pristine electrolyte, 0.1 wt% nanofluidic electrolyte increased energy
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storage capacity 26.0 to 31.7 Ah L-1 after 62 cycles which corresponded to 22% increase. The
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nanofluidic electrolytes exhibited a breakthrough that ensures high energy storage capacity and
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electrochemical efficiency by increasing the reversibility of VRFB, maintaining most of the 15
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existing facilities, and securing energy capacity by a convenient method. In addition, we plan
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to use our single-cell evaluation of nanoparticles containing various carbon or functional
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groups.
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Acknowledgments
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This research was supported by Basic Science Research Program through the National Research
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Foundation of Korea funded by the Ministry of Education (No. 2015R1D1A3A01019588) and the
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National Research Foundation of Korea grant funded by the Korea government (No. NRF-
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2017M1A3A3A02016566).
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Energy storage capacity increased by nanofluidic electrolyte. Electrochemical activity and reversibility increased by MWCNT. Nanofluidic electrolyte with 0.1 wt% of MWCNT enhances 22 % of specific discharge capacity.