Impact of nanofluidic electrolyte on the energy storage capacity in vanadium redox flow battery

Impact of nanofluidic electrolyte on the energy storage capacity in vanadium redox flow battery

Accepted Manuscript Impact of nanofluidic electrolyte on the energy storage capacity in vanadium redox flow battery Jungmyung Kim, Heesung Park PII: ...

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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

This is a PDF file of an unedited manuscript that has been accepted for publication. As a service to our customers we are providing this early version of the manuscript. The manuscript will undergo copyediting, typesetting, and review of the resulting proof before it is published in its final form. Please note that during the production process errors may be discovered which could affect the content, and all legal disclaimers that apply to the journal pertain.

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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

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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

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reaction performance is proportional to the content of MWCNT in nanofluidic electrolytes. The

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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

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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

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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

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demand/supply and limited conditions of large-scale power utility [1,2]. The energy storage

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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,

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high energy efficiency, long lifetime, and free from cross-over contamination [4-6]. Various

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redox couples [7], cell components [8,9], and optimum operating conditions [10,11] have been

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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

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applications [12], there still requires a breakthrough technology to overcome low energy

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storage density of VRFB. Zhang et al. have shown that the discharge capacity of VRFB was

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enhanced by effectively mixing the electrolyte [13]. Nonetheless, lithium-ion battery offers up

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to 500 Wh L-1 whereas VRFB does 33 Wh L-1 due to the limited solubility of vanadium species

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(1-2 M) [14,15]. Therefore, a progressive technology is required to overcome the limitation of

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energy storage density in VRFB.

50

On the other hand, novel approaches to energy efficiency and capacity enhancement have

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been investigated, most of which have demonstrated increased electrochemical properties

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using nano-sized materials. Especially, nanoparticles have drawn attention to increase

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electrochemically active sites of carbon felt electrode in VRFBs. Bismuth nanoparticles [16]

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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

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nanotubes served an electrode catalyst for VRFBs. Wu et al. proposed cost effective and a high-

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performance electrode by growing N-doped carbon nano-spheres on graphite felt fibres [19].

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They demonstrated the superior performances of energy efficiency and capacity retention by

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conducting single cell test. Li et al. investigated carbon electrode with hollow nanofibers which

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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

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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,

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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

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electrochemical performance and energy storage capacity by dispersing nano-sized materials

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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

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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,

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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)

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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

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0.1 weight percent (wt%) MWCNT is found to retain specific discharge capacity of 31.7 Ah

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L-1 which is 22% higher than pristine electrolyte.

80 81 82

2. Experimental 2.1 Characterization of materials

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The nanostructures of MWCNTs were analyzed by field emission transmission electron

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microscopy (TEM, JEM 2100F, JEOL) and X-ray diffractometer (D8 Discover, BRUKER)

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operated at 160-200 kV and 40 kV, respectively. Raman spectroscope (JP/NRS-3300, JASCO)

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equipped with a 100 mW solid-state primary laser at 532 and 785 nm was used to identify the

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compositions of the materials. The surface morphologies of carbon felt electrodes were

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inspected by using a field emission scanning electron microscope (SEM, Merlin compact,

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ZEISS) operating at 5 kV. Optical microscope (JP-E600, Nikon) was also used to visualize the

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dispersion of MWCNTs in nanofluidic electrolytes.

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2.2 Preparation of nanofluidic electrolytes

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The pristine electrolyte used in the experiments was prepared by electrochemical

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decomposition of 1.6 M VOSO4 and 4 M H2SO4 solution [26]. The positive and negative

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electrolytes were divided into electrolytes of different valence states (V3+/VO2+) after

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conducting 40 mA cm-2 constant current on 10 charge/discharge cycles. With these electrolytes,

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different wt% MWCNT nanofluidic electrolyte were produced to secure experimental

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consistency. Graphene has a hexagonal carbon ring bond of carbon atoms in a two-dimensional

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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-

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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)

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with length ranging from 10 to 20 μm were supplied by Carbon Nanotubes Plus, USA, with

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specifications as listed in Table 1. Fig. 1a and b show the TEM and SEM images of a single

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MWCNT and MWCNT powder, respectively. The multiple graphitic edge planes of MWCNTs

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can be observed in the image. As shown in Fig. 1c and d, three different weights of MWCNT

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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

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that the temperature of sonicator was kept at 23 ± 1 °C to prevent unwanted precipitation of

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the electrolyte as illustrated in Fig. 1e. The dispersion of nanofluidic electrolytes was visually

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inspected by optical microscopy as displayed in Fig. 1f. It can be seen that the MWCNTs were

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homogeneously dispersed for all nanofluidic electrolytes.

113

114 115

Fig. 1. Schematic diagram of manufacturing process of nanofluidic electrolytes; (a) TEM (b)

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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

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by using cyclic voltammetry (CV, NuVant System, Powerstat-05) test with three electrodes.

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Electric potential variations were recorded by using a saturated silver-silver chloride double-

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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

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used in the test was 15 mL for all cases. The applied scan rate was varied from 5 to 200 mV s-

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1

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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,

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2.4 Single cell test

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The VRFB single cell with 25 cm2 of active area was composed of polytetrafluoroethylene

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gaskets, bipolar plates (BLUE 100-BP, Standard Energy), 4.6 mm thickness carbon felt

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electrodes (SIGRACELL, GFD 4.6 EA, SGL) in thickness of 3 mm after compression, a Nafion

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membrane (NR-117) and an oxygen-free copper current collecting plates as illustrated in Fig.

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2 [26]. In order to improve the electrical conductivity, corrosion resistance and brittleness of

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copper, oxygen-free copper prepared so that the oxygen content is 0.008% or less through

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deoxidizing agent was used. The cell was connected with a power supply (Sorensen HPD series,

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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

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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

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0.5 MPa between two endplates. With this, it was confirmed that the sealing of the single cell

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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

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experiments of charge/discharge cycles were conducted by applying constant electrical current

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of 120 mA cm-2. After the completion of experiments, the used carbon electrodes were taken

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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

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nanofluidic electrolytes in the active area.

155 156 157

3. Results and discussion 3.1. Physico-chemical analysis

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The X-ray diffraction patterns of MWCNT and carbon felt electrode are depicted in Fig. 3a.

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It can be seen that the peak intensities of 2θ = 25.6 ° and 2θ = 23.9 ° reflect the graphite

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composition of (002) and (100), respectively. Fig. 3b compares the Raman spectra of MWCNT

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and carbon felt electrode. The D bands (first peak) of the two materials were commonly

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presented at 1340 cm-1. Since the D band reflected the content of graphitic edge which became

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the active sites (defects) of the graphite materials [15], it could be expected that the presented

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D band in MWCNT increased the active sites during the electrochemical reaction in VRFB.

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Furthermore, the G band (second peak) commonly was found at 1580 cm-1. The intensity ratio

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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

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MWCNT.

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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

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and 7.481 mPa s for pristine, 0.05, 0.1 and 0.2 wt% electrolyte, respectively. The increment of

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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 –

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5.08 mPa s were very close to that measured by Li et al. [28]. Nonetheless, significant increase

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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

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To investigate the effect of nanofluidic electrolyte on the electrochemical reaction, CV tests

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were performed for positive (VO2+/VO2+) and negative (V2+/V3+) electrolytes with 0 (pristine),

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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

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V (negative electrolyte). For both of the positive and negative electrolyte, the measured

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oxidation-reduction peak current densities were in the order of MWCNT content. The increased

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peak current density was caused by the improved electron transfer kinetics of VO2+/VO2+ and

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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

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area and the active interface provided by conventional electrodes. The increased active sites of

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nanofluidic electrolyte also improved the oxidation potential from 1.066 V (0 wt%) to 1.028 V

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(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-

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reduction potential difference. Furthermore, the peak current density variations with respect to

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different nanofluidic electrolytes and scan rates are presented in Fig. 4c and d. The peak current

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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

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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

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transfer rate. In this, the nanoparticles in the nanofluidic electrolyte enhanced the

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electrochemical performance through a double layer mechanism.

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The peak current densities (Ipox and Ipre, for oxidation and reduction, respectively), ratios of

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peak current density (Ipox/Ipre) and oxidation-reduction peak potential differences (ΔEp) are

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summarized in Table 2. Although peak current density increased with MWCNT content in

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electrolyte, the minimum ratio of peak current density and peak potential difference were 1.38

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and 0.14 V for 0.1 wt% positive nanofluidic electrolyte. Nonetheless, minimum peak potential

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difference was presented when 0.05 wt% MWCNT negative nanofluidic electrolyte was used.

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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

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test was also carried out to further investigate the effect of MWCNT content in electrolyte on

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the long-term stability.

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30

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 )

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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

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50 charge/discharge cycling test. Fig. 5a shows that the peak current densities of positive

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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

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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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271

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

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62nd cycle was 0.4, 0.18, 0.18 and 0.3 % per cycle for the same order of MWCNT concentration

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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)

305

(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

314

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.

331 332

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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References [1] Ferreira HL, Garde R, Fulli G, Kling W, Lopes JP. Characterisation of electrical energy storage technologies. Energy 2013;53:288–98.

342

[2] Liu J, Zhang JG, Yang Z, Lemmon JP, Imhoff C, Graff GL, et al. Materials science and materials chemistry

343

for large scale electrochemical energy storage: From transportation to electrical grid. Adv Funct Mater

344

2013;23:929–46.

345 346 347 348

[3] Yin C, Gao Y, Guo S, Tang H. A coupled three dimensional model of vanadium redox flow battery for flow field designs. Energy 2014;74:886–95. [4] Wang W, Luo Q, Li B, Wei X, Li L, Yang Z. Recent progress in redox flow battery research and development. Adv Funct Mater 2013;23:970–86.

349

[5] Cunha Á, Brito FP, Martins J, Rodrigues N, Monteiro V, Afonso JL, et al. Assessment of the use of vanadium

350

redox flow batteries for energy storage and fast charging of electric vehicles in gas stations. Energy

351

2016;115:1478–94.

352 353 354 355 356 357 358 359 360 361 362 363 364 365 366 367 368 369 370 371 372 373 374 375

[6] Skyllas-Kazacos M, Chakrabarti MH, Hajimolana SA, Mjalli FS, Saleem M. Progress in Flow Battery Research and Development. J Electrochem Soc 2011;158:R55. [7] Wang W, Kim S, Chen B, Nie Z, Zhang J, Xia G-G, et al. A new redox flow battery using Fe/V redox couples in chloride supporting electrolyte. Energy Environ Sci 2011;4:4068. [8] Liu Q, Sleightholme AES, Shinkle AA, Li Y, Thompson LT. Non-aqueous vanadium acetylacetonate electrolyte for redox flow batteries. Electrochem Commun 2009;11:2312–5. [9] Wei L, Zhao TS, Zhao G, An L, Zeng L. A high-performance carbon nanoparticle-decorated graphite felt electrode for vanadium redox flow batteries. Appl Energy 2016;176:74–9. [10] Pan J, Huang M, Li X, Wang S, Li W, Ma T, et al. The performance of all vanadium redox flow batteries at below-ambient temperatures. Energy 2016;107:784–90. [11] Badrinarayanan R, Tseng KJ, Soong BH, Wei Z. Modelling and control of vanadium redox flow battery for profile based charging applications. Energy 2017;141:1479–88. [12] Dunn B, Kamath H, Tarascon JM. Electrical energy storage for the grid: A battery of choices. Science (80- ) 2011;334:928–35. [13] Zhang Y, Liu L, Xi J, Wu Z, Qiu X. The benefits and limitations of electrolyte mixing in vanadium flow batteries. Appl Energy 2017;204:373–81. [14] Akinyele DO, Rayudu RK. Review of energy storage technologies for sustainable power networks. Sustain Energy Technol Assessments 2014;8:74–91. [15] Dubal DP, Gomez-Romero P. Electroactive graphene nanofluids for fast energy storage. 2D Mater 2016;3:31004. [16] Li B, Gu M, Nie Z, Shao Y, Luo Q, Wei X, et al. Bismuth nanoparticle decorating graphite felt as a highperformance electrode for an all-vanadium redox flow battery. Nano Lett 2013;13:1330–5. [17] Li B, Gu M, Nie Z, Wei X, Wang C, Sprenkle V, et al. Nanorod niobium oxide as powerful catalysts for an all vanadium redox flow battery. Nano Lett 2014;14:158–65.

376

[18] Li W, Liu J, Yan C. The electrochemical catalytic activity of single-walled carbon nanotubes towards

377

VO2+/VO2+ and V3+/V2+ redox pairs for an all vanadium redox flow battery. Electrochim Acta 17

ACCEPTED MANUSCRIPT

378 379 380 381 382

2012;79:102–8. [19] Wu L, Shen Y, Yu L, Xi J, Qiu X. Boosting vanadium flow battery performance by Nitrogen-doped carbon nanospheres electrocatalyst. Nano Energy 2016;28:19–28. [20] Li L, Peng S, Lee JKY, Ji D, Srinivasan M, Ramakrishna S. Electrospun hollow nanofibers for advanced secondary batteries. Nano Energy 2017;39:111–39.

383

[21] Di Blasi A, Busaccaa C, Di Blasia O, Briguglioa N, Squadritoa G, Antonuccia V. Synthesis of flexible

384

electrodes based on electrospun carbon nanofibers with Mn3O4 nanoparticles for vanadium redox flow

385

battery application. Appl Energy 2017;190:165–71.

386

[22] El-Seesy AI, Abdel-Rahman AK, Bady M, Ookawara S. Performance, combustion, and emission

387

characteristics of a diesel engine fueled by biodiesel-diesel mixtures with multi-walled carbon nanotubes

388

additives. Energy Convers Manag 2017;135:373–93.

389

[23] Al-Shamani AN, Alghoul MA, Elbreki AM, Ammar AA, Abed AM, Sopian K. Mathematical and

390

experimental evaluation of thermal and electrical efficiency of PV/T collector using different water based

391

nano-fluids. Energy 2018;145:770–92.

392

[24] Sadeghinezhad E, Mehrali M, Saidur R, Mehrali M, Tahan Latibari S, Akhiani AR, et al. A comprehensive

393

review on graphene nanofluids: Recent research, development and applications. Energy Convers Manag

394

2016;111:466–87.

395 396 397 398 399 400 401 402 403 404 405 406 407 408

[25] Timofeeva EV, Katsoudas JP, Segre CU, Singh D. Rechargeable Nanofluid Electrodes for High Energy Density Flow Battery. NSTI-Nanotech 2013;2:679–82. [26] Kim J, Park H. Experimental analysis of discharge characteristics in vanadium redox flow battery. Appl Energy 2017;206:451–7. [27] Wang S, Zhao X, Cochell T, Manthiram A. Nitrogen-doped carbon nanotube/graphite felts as advanced electrode materials for vanadium redox flow batteries. J Phys Chem Lett 2012;3:2164–7. [28] Li X, Xiong J, Tang A, Qin Y, Liu J, Yan C. Investigation of the use of electrolyte viscosity for online stateof-charge monitoring design in vanadium redox flow battery. Appl Energy 2018;211;1050-59. [29] Kabtamu DM, Chen J-Y, Chang Y-C, Wang C-H. Water-activated graphite felt as a high-performance electrode for vanadium redox flow batteries. J Power Sources 2017;4:11472–80. [30] Pour N, Kwabi DG, Carney T, Darling RM, Perry ML, Shao-Horn Y. Influence of edge-and basal-plane sites on the vanadium redox kinetics for flow batteries. J Phys Chem C 2015;119:5311–8. [31] Wang K, Liu L, Xi J, Wu Z, Qiu X. Reduction of capacity decay in vanadium flow batteries by an electrolyte-reflow method. J. Power Sources 2017;338;17-25.

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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.