J Po lue ran sael od fo Mn aot te rai ad l js u Cs ht emm ai rs gt ri yn sA
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respectively(Fig. S17b and Fig. S18b), showing that the existence of
Al . The C spectra has a main peaks of 284.9eV for compound 1
and 284.59eV for compound 2, respectively(Fig. S17c and Fig. S18c),
which belongs to the C1s. The N1s spectrum48 is divided into two
i = avb
(1)
DOI: 10.1039/C9TA14103K
3
+
where a and b are the coefficients, i is the peak current density(A),
-1
and v is the scan rate (mV s ). The calculated value of b can be
distributed into capacitive and diffusion controlled charge
contributions for the charge storage mechanism in the electrode
peaks(Fig. S17d and Fig. S18d), which can be attributed to the -N=
+
and-NH -/-NH-fragments (399.38 and 401.68eV for compound 1
material. If b=0.5 (i∞v1/2) for the diffusion-controlled charges (Q
and b=1 (i∞v) for the surface capacitive (Q ). As shown in Fig. S24
and Fig.3c, good linear relationship is observed between
log(current density) and log(scan rate) for Na 40-, 1- and 2-
CC electrodes and and the b values are observed to be 0.93, 0.92,
and 0.90, respectively. The larger b value of these electrodes
indicated the kinetics behaviors are mainly quite attributed to the
d
)
and 399.2 and 401.6eV for compound 2). The O1s spectra reveal the
co-existence of C-O and C=O (532.08 and 531eV for compound 1
and 532.1 and 531eV for compound 2). Furthermore, the Ag3d
spectrum has two main peaks of 368.08 and 374.08eV for
compound 1, and they can clearly demonstrate the existence of Ag+
s
a
5
AlW12O
(
9
Figure S17e). In addition, the Cu2p spectrum has a main peak at the
32.9eV, and the existence of Cu (Fig. S18e) for compound 2.
+
40
surface layer capacitance due to the redox reaction of {AlW12O }
and the pseudocapacitances from the transformation of W (W to
As shown in Fig.S19a, S21a, the SEM of compounds 1 and 2 show
the morphology of block shape and the length and width of 400µm
6
+
5
+
W ).
×
297µm for compound 1 and 314µm × 107µm for compound 2,
respectively. EDS microanalysis of compounds 1 and 2 were shown
in Fig.S19b, S21b, which can be clearly seen in that the elements O,
C, Al, Cu(or Ag), N, and W were existenced. At the same time,
mapping diagram(Fig.S20 and S22) further confirmed that the
composition of compounds 1-2 were equably distributed.
At the same time, we further studied and separated the
contributions of capacitive and diffusion controlled charge from the
total charge storage(Q), using an approach reported elsewhere :
7
6
Q=Q +Q (2)
c
d
The contribution of Q
surface adsorption, which is the combination of a false capacitance
and a double-layer capacitor, and the contribution of Q is the
redox reaction ascribed to the electrode materials. Supposing the
semi-infinite linear diffusion processes at a fixed potential, Q is
obtained by plotting the stored charge(Q) vs. the reciprocal of the
square root of the scan rate and Q vary according to the scan rates.
c
is related to the scan rate, mainly due to
Electrochemical measurements
Cyclic voltammetry studies
d
The unique polymer chains, the small molecule ligands of
ethylenediamine, and multi-electron transfer process of
c
Na
potential applications in SCs. Three-electrode cyclic voltammetry
CV) curves at the 20 mV s-1 scan rate in 0.5M H
SO are presented
5
AlW12O40-, 1- and 2-CC provoke us to further investigate their
d
Hence, the total charge stored can be represented by the following
equation:
(
2
4
in Fig. 3a. The specific capacitances of these compounds are
correlated to the average areas of the CV curves which follow the
Q= Q
c
+ kv1/2
(3)
order of 2-CC> 1-CC> Na
polyanions, the specific capacitances of 2-CC with {-4,4’-bipy-Cu-4,4’
bipy} polymer chains and small-molecule ethylenediamine ligands
are much higher than 1-CC with {-4,4’-bipy-Ag-4,4’-bipy} , and the
capacitance of the Na 40 is the smallest of the three
compounds. These results clearly demonstrate that the specific
capacitances of {AlW12} materials are related to the polymer chains
and small-molecule ligands as well as their structural features. Fig.
S23 and Fig. 3b show the CV curves of 1-CC and 2-CC with a
potential window from -0.2 to 0.9 V at different scanning rates.
Clearly, 1-CC and 2-CC show the quadrilateral shape with a pair of
redox peaks, indicating the coexistence of both the electrical
double-layer capacitance and pseudocapacitance. With the increase
of scan rates, the current response is likewise gradually increased,
exhibiting good capacitive behaviour and charge storage
characteristics.
5
AlW12O40-CC. With the same {AlW12}
Where k is a constant. Fig. S25(a-c) are the linear diagram of Q and
the square root reciprocal of the scan rate(v-1/2) for Na
- and 2-CC electrodes, shown that the storage charge ability of 2-
CC is the strongest and consistent with the CVs. Q and Q are
5
AlW12O40-,
-
n
1
n
c
d
5
AlW12O
estimated and plotted in Fig.S26 and Fig.3(d), demonstrated the
normalized contribution ratio of capacitive and diffusion controlled
-1
charge storage capacities at 5-100 mV s . There are clearly seen
that the diffusion-controlled process contribution decreases
-1
gradually with increasing the scan rate (from 5 to 100 mV s ), while
the contribution of Q increases. Obviously, Q is more prominent in
c
c
these electrode materials and it shows the pseudocapacitive nature
of the electrodes.
In our view, 1- and 2-CC all show similar CV curves due to their
40]5-. Since the open
similar structures on the base of same [AlW12
O
metal sites of {AlW12} polyanions all are occupied by {-4,4’-bipy-M-
,4 ’ -bipy} (M= Ag, Cu) polymer chains or small-molecule
4
n
To further analyze the total charge storage (capacitive and diffusion
controlled charge contributions) of Na AlW12O40-, 1- and 2-CC
5
electrodes were achieved by estimating the current response of CV
curves. It is known that the peak current usually follows the power
law relationship with the scan rates. As showed in equation (1):
ethylenediamine ligands. H+ ions of electrolytes can continuously
attack polyoxoanion, and its auxiliary redox process at the open
metal center is suitable. Under this experimental condition, {AlW12
}
clusters may provide an effective electron transfer with inner-
4
| J. Name., 2012, 00, 1-3
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