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The working principle of the BB3/V ARFB is illustrated in Figure (Figure S5). Therefore, it is inferred that heteroatom nitrogen
1. BB3 is one of typical phenoxazinum derivatives, in which plays an important role in the redoxDpOrI:o1c0e.1s0s39f/oDr0CBCB03513o3nK
three heterocyclic frameworks provide a stably π-conjugated GC@NG.38
system, and p-π electron donating conjugated effect of two
nitrogen atoms makes a steady resonance structure.31 The
heteroatom oxygen increases the electron affinity of the
molecules, and thus improves the redox potentials to meet the
catholyte demand.30 The redox reactions of BB3 take place with
two electrons and two protons in one step to balance the
charge with the extra positive charge locating at the nitrogen
atom of the side ammonium group.32 Compared to single
electron transfer molecules, BB3 with two-electron transfers
can efficiently improve the battery capacity.
High solubility of the redox active materials is desired to
achieve high capacity of the full battery. As calculated via the
capacity formula in supporting information, ARFBs with organic
electrolyte require an equivalent electron concentration of at
least 1.5 M to reach a competitive capacity with all-vanadium
ARFBs (~40 Ah/L). In this work, BB3 receives a maximum
solubility of 2.5 M in mixed solvent (H2O+HoAc volume ratio of
1:1, containing 3.5 M H2SO4) measured by UV-vis (Figure S2).
Figure 2. (a) SEM image of the morphology of pure NG. (b) XPS spectrum and (c) N1s high
Considering its ability to store two electrons per molecule, this
solubility corresponds to a theoretical equivalent electron
concentration of 5.0 M and charge capacity of 134 Ah/L. The
high solubility can be attributed to the hydrophilic tertiary
amines group at both side chains of BB3. In addition, HoAc has
been demonstrated as an useful cosolvent,30 which can
significantly increase the solubility of BB3. Fourier-transform
infrared spectroscopy (FTIR) spectra further proves that there is
only some negligible structure change for BB3 in the mixed
supporting solution (Figure S3).
CV curve was performed with bare glass carbon (bare GC)
electrode in electrochemical workstation to investigate the
electrochemical reversibility of BB3. As shown in Figure S4, the
redox process of BB3 is acidity dependent due to the
protonation/deprotonation of BB3 involved in the redox
reaction. The result indicates an apparent CV curve with a redox
potential of 0.54 V vs SHE in 3.5 M H2SO4 as supporting solution.
ΔE from CV curve is an useful parameter to estimate the redox
dynamics of active species.33 The CV curve of BB3 with a large
ΔE reveals sluggish redox kinetics, which might lead to a
decrease of energy efficient by creating large over potentials in
the full battery.33, 34
In order to overcome the drawback of the sluggish kinetics,
various nanomaterials have been used to catalytic the redox
process of the active species.35-37 In this work, we introduced
NG as an electrocatalyst to modify the bare GC electrode,
named as GC@NG. The three-dimensional morphology of NG
can supply more active sites for redox reaction (Figure 2a).38 The
high concentration of nitrogen atoms (6.5 at.%, Figure 2b-c) is
in favour of superior catalytic activity for the BB3 redox
reaction. As shown in Figure 2d, the ΔE significantly reduces to
63 mV from 308 mV, indicating a remarkable catalytic effect.
Previous work have shown that nanocarbon materials could
effectively catalyze the redox process.39-41 However, in this
work, there is no obvious improvement obtained for the BB3
redox process on pure graphene modified bare GC electrode
resolution spectra of pure NG. (d) CV curves of 0.05 M BB3 in 3.5 M H2SO4 under 0.1 V/s
on bare GC and GC@NG, respectively.
The dynamic parameters of BB3 during redox process were
measured by linear sweep voltammetry (LSV) on a rotating disk
electrode device with the rotations from 400 to 2500 rpm. The
LSV curves were obtained by sweeping from the positive to
negative potentials on bare GC (Figure S6) and GC@NG (Figure
S7) electrodes, respectively. For bare GC electrode, typical
sigmoidal LSV curves show one wave at ~0.45 V (Figure S6a),
indicating a one-step reaction in the reduction process of BB3.
In contrast, GC@NG electrode shows two waves at ~0.40 and
~0.52 V in its LSV curves. The low potential wave is rotation-
dependent, representing the reduction process of BB3. The
higher one is rotation-independent (Figure S7a-b), suggesting
the adsorption process of BB3 on GC@NG, which is further
confirmed by the LSV measurements from the reversed
sweeping direction (Figure S8). The disappearance of the high
potential wave at ~0.52 V in the positive sweeping (Figure S8,
S7c-d) could be attributed to the consumption of absorbed BB3.
Clearly, the LSV measurement performed under none-
adsorption condition is a better way to determine the diffusion
coefficient (D0) and redox constant rate (k0) of redox materials.
According to the Levich equation,33 the D0 of BB3 in the bulk
solution is 1.1×10-7 cm2 s-1. The redox constant rate k0 of BB3 on
GC@NG calculated through Koutecky-Levich equation is
2.87×10-3 cm s-1, which is about 1.5 times greater than that on
the bare GC electrode (1.95×10-3 cm s-1), revealing that NG
effectively facilitates the BB3 redox reaction.
By pairing with V2+/V3+ as anolyte, two BB3/V ARFBs were
constructed with 0.05 M BB3 in 3.5 M H2SO4 as catholyte using
bare carbon paper (bare CP) and NG modified CP (CP@NG) as
working electrode, respectively. Compared with bare CP based
battery, the CP@NG based battery displays lower
overpotentials and higher battery capacity, even at high current
densities (Figure 3a, b). Since the resistances of the two
2 | J. Name., 2012, 00, 1-3
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