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. 2018 Apr 23;18:1448–1456. doi: 10.1016/j.dib.2018.04.057

Data on high performance supercapacitors based on mesoporous activated carbon materials with ultrahigh mesopore volume and effective specific surface area

Yanhong Lu a,, Suling Zhang a, Jiameng Yin a, Congcong Bai a, Junhao Zhang a, Yingxue Li a, Yang Yang b, Zhen Ge b, Miao Zhang b, Lei Wei a, Maixia Ma a, Yanfeng Ma b, Yongsheng Chen b,
PMCID: PMC5997976  PMID: 29904649

Abstract

The data presented in this data article are related to the research article entitled “Mesoporous activated carbon materials with ultrahigh mesopore volume and effective specific surface area for high performance supercapacitors” (Lu et al., 2017) [1]. The detailed structure data of the prepared mesoporous activated carbon materials with ultrahigh mesopore volume and effective specific surface area and the electrochemical performance data of the corresponding supercapacitors are described.


Specifications Table

Subject area Chemistry
More specific subject area Materials science: activated carbons (ACs)
Type of data Table, image, text file, graph, figure and video
How data was acquired X-ray photoelectron spectroscopy (XPS) spectrometer (AXIS HIS 165, Kratos Analytical); Nitrogen isotherm of N2 at 77 K (Micromeritics ASAP 2020); CHI660C electrochemical analyzer (Shanghai Chenhua Instruments Co., Ltd.); Battery test system (LAND CT2001A model, Wuhan LAND Electronics. Ltd.); P4000 electrochemical workstation (Princeton, USA)
Data format Raw and analyzed
Experimental factors Samples, assembled coin-type supercapacitor and calculation
Experimental features Characterization of electrode material, assembly of device and measurement of electrochemical performance
Data source location Langfang Normal University and Nankai University, China
Data accessibility Data are presented in this article

Value of the data

  • Detailed experimental data and procedures might be used for further scientific development and further studies.

  • Surface element composition data and pore size distribution curves could be used for more scientific analysis of the microstructure of carbon materials, and helpful for material design and optimization.

  • The calculation method for effective specific surface area and theoretical capacitance could be used to evaluate reliably the material's performance used for double layer electrochemical capacitor without fabricating real and industry standard devices.

  • Electrochemical performance data of other materials including the reference material than the optimal material can be used to compare together and used for the optimization of material design.

1. Data

In this data article, the detailed structure and electrochemical data of the prepared mesoporous activated carbon materials (AC-KOH) and the control samples are presented. The data include the surface element composition (Table 1), pore size distribution (PSD) curves (Fig. 1), the calculation method of the effective specific surface (E-SSA) (Table 2), the electrochemical performance data in organic (TEABF4/AN), aqueous (KOH) and ion liquid (EMIMBF4) electrolyte systems (Fig. 2, Fig. 3, Fig. 4, Fig. 5). The photograph and video for lighting a LED using the AC-KOH based supercapacitor are demonstrated (Fig. 6). In addition, the structure and electrochemical data of the optimal material AC-KOH and other reported materials are also summarized (Table 3).

Table 1.

Element composition of AC-KOH and the control commercial YP50 by XPS analysis.

Sample C (at%) N (at%) O (at%)
AC-KOH 94.46 0.67 4.87
YP50 94.06 0.51 5.43

Fig. 1.

Fig. 1

Pore size distribution of a series of prepared ACs with different activation agents/ratios and the compared commercial YP50 based on the NL-DFT method from the nitrogen adsorption data.

Table 2.

Detailed data for the calculation of E-SSA for AC-KOH electrode material.

Wa(nm) DFT SSA (m2g-1) Db(nm) E-SSA (m2g-1)
0.500 0 0.684 0
0.536 0 0.684 0
0.590 0 0.684 0
0.643 0 0.684 0
0.679 0 0.684 0
0.733 97 0.684 97
0.804 65 0.684 65
0.858 0 0.684 0
0.929 0 0.684 0
1.001 0 0.684 0
1.090 113 0.684 113
1.179 272 0.684 272
1.269 75 0.684 75
1.358 38 1.32 38
1.483 39 1.32 39
1.591 15 1.32 15
1.716 15 1.32 15
1.859 14 1.32 14
2.002 9 1.32 9
2.162 41 1.32 41
2.341 68 1.32 68
2.520 88 1.32 88
2.734 115 1.32 115
2.949 98 1.32 98
3.181 96 1.32 96
3.431 110 1.32 110
3.699 85 1.32 85
4.003 76 1.32 76
4.325 67 1.32 67
4.664 53 1.32 53
5.040 42 1.32 42
5.433 29 1.32 29
5.880 20 1.32 20
6.344 12 1.32 12
6.845 7 1.32 7
7.399 3 1.32 3
7.988 2 1.32 2
8.632 2 1.32 2
9.311 2 1.32 2
10.061 1 1.32 1
10.866 1 1.32 1
11.723 1 1.32 1
12.653 0 1.32 0
13.671 0 1.32 0
14.761 0 1.32 0
15.941 0 1.32 0
17.210 0 1.32 0
18.586 0 1.32 0
20.069 0 1.32 0
21.660 0 1.32 0
23.393 0 1.32 0
25.252 0 1.32 0
27.271 0 1.32 0
29.451 0 1.32 0
31.792 0 1.32 0
34.330 0 1.32 0
37.064 0 1.32 0
40.031 0 1.32 0
43.230 0 1.32 0
46.679 0 1.32 0
50.396 0 1.32 0
54.417 0 1.32 0
58.760 0 1.32 0
63.442 0 1.32 0
68.499 0 1.32 0
73.968 0 1.32 0
79.865 0 1.32 0
86.245 0 1.32 0
93.126 0 1.32 0
100.560 0 1.32 0
108.566 0 1.32 0
117.233 0 1.32 0
126.580 0 1.32 0
136.677 0 1.32 0
147.596 0 1.32 0

Wa: pore width of the electrode material.

Db: diameter of the effective electrolyte ion.

Fig. 2.

Fig. 2

Capacitance performance of the supercapacitor with prepared AC-KOH and commercial YP50 in TEABF4/AN electrolyte system tested at current densities from 0.5 to 2 A g-1.

Fig. 3.

Fig. 3

Galvanostatic charge/discharge curves for AC-KOH based supercapacitor tested at current density of 5, 10, 15, 20 and 30 A g-1, respectively.

Fig. 4.

Fig. 4

Electrochemical performance of AC-KOH and YP50 based supercapacitors in 6 M KOH electrolyte system. (a) CV curves of AC-KOH based supercapacitor measured at the scan rates of 5, 10 and 20 mV s-1 in the potential range of 0−1.0 V. (b) Galvanostatic charge/discharge curves for AC-KOH based supercapacitor tested at current densities from 0.1 to 2 A g-1. (c) Rate performances and (d) Nyquist plots of AC-KOH and YP50 based supercapacitors. The inset in (d) is the enlarged one of the rectangular region.

Fig. 5.

Fig. 5

Galvanostatic charge/discharge curves for AC-KOH and YP50 based supercapacitors in EMIMBF4 electrolyte system tested at current density of 1 A g-1.

Fig. 6.

Fig. 6

The optical images of a red LED before and after lightened by a charged supercapacitor with AC-KOH as the electrode material and EMIMBF4 as the electrolyte.

Table 3.

The structure and capacitive performance comparison between AC-KOH prepared in this work and other typical biomass derived ACs reported in literatures.

Biomass SSA (m2g-1) Total pore volume (cm3g-1) Vmicro(cm3 g-1) Vmeso(cm3 g-1) Cp(F g-1) Ref.
egg white 3250 1.97 184 in LiPF6 [4]
ramie fiber 2087 1.08 0.43 0.65 287 in KOH [5]
cotton fabric 777 0.2 184 in KOH [6]
bamboo 1293 0.634 0.429 0.205 [7]
prosopis juliflora 2410 1.196 1.120 0.076 160 in LiPF6 [8]
sucrose 2953 1.26 1.03 0.23 160 in H2SO4 [9]


 

 

 

 

 

 


cornstalk core 2139 1.16 317 in KOH [10]
E = 6.8 W h kg-1
P = 28.3 kW kg-1
sugar cane bagasse 2289 1.358 0.237 1.046 [11]
Starch 1157 0.97 0.05 0.92 144 in KOH [12]


 

 

 

 

 

 


poplar catkins 1400 206 in aqueous electrolyte [13]
E = 7.5 W h kg-1


 

 

 

 

 

 


pollen 3037 2.27 0.41 1.86 207 in AN [14]
E = 88 W h kg-1
prosopis juliflora 2448 1.2116 1.1191 0.0925 [15]
corn grains 3199 1.645 1.015 0.63 257 in KOH [16]


 

 

 

 

 

 


corncob 3054 1.50 0.738 0.762 328.4 in KOH [17]
401.6 in H2SO4
acacia gum 1832 1.04 0.84 0.20 272 in KOH [18]
corn stover 1671.4 0.831 0.634 0.197 236.4 in KOH [19]
coconut kernel 1200 0.605 0.457 173 in H2SO4 [20]
potato starch 2342 1.24 1.08 0.16 335 in KOH [21]
cow dung 1984 0.91 0.62 0.29 125 in AN [22]
microalgae 2130 0.90 0.84 0.06 200 in LiCl [23]
green needle coke 3347 1.8 348 in KOH [24]
Sucrose 1941 0.919 0.874 0.045 148 in EMIMBF4 [25]
β-cyclodextrin 781 0.41 0.27 0.14 157 in KOH [26]
dragon fruit skin 911 0.47 0.25 0.22 286.9 in KOH [27]


 

 

 

 

 

 


corn straw 3237 2.27 0.42 1.85 222 in KOH this work
202 in TEABF4/AN
188 in EMIMBF4
E = 80 W h kg-1
P = 870 W kg-1

2. Experimental design, materials and methods

AC-KOH and the control materials (AC-ZnCl2, AC-K2CO3, AC-Na2CO3, AC-KOH-2:1 and AC-KOH-5:1) were prepared through a hydrothermal carbonization and followed by an activation process using biomass straw as the raw material. A control carbon material, commercial activated carbon YP50, was obtained from Tianjin Plannano Energy Technologies Co., Ltd. The surface element composition of AC-KOH and YP50 was measured through XPS analysis using AXIS HIS 165 spectrometer (Kratos Analytical) with a monochromatized Al Kα X-ray source (1486.71 eV photons). As shown in Table 1, the contents of C and O elements in AC-KOH were estimated as 94.46% and 4.87% respectively, similar to that of commercial YP50. The PSD data of AC-KOH and the control carbon materials were obtained using the Brunauer-Emmett-Teller (BET) analysis and the density functional theory (DFT) method. Based on the PSD data, together with the cumulative DFT SSA and the electrolyte ion size, the E-SSA of electrode material was calculated. The electrochemical performance data, including cyclic voltammetry curves (CV), galvanostatic charge-discharge curves and cycling stability data, was obtained through assembled symmetrical coin-type supercapacitor.

Based on the PSD data of AC-KOH, together with the cumulative DFT SSA and the electrolyte ion size, the E-SSA of electrode material was calculated. The detailed data is shown in Table 2. The data of DFT SSA was obtained from the BET analysis directly. For TEABF4/AN electrolyte, the solvent free/bare TEA+ ion (diameter of 0.684 nm) and solvated TEA+ ion (diameter of 1.32 nm) were used for the E-SSA calculation [2], [3]. When the pore width of the carbon material is larger than 0.684 nm but smaller than 1.32 nm, the size of bare TEA+ ion was used for the calculation. While when the pore width of the carbon material is larger than 1.32 nm, the size of solvated TEA+ ion was used for such calculation. These two parts were then added together as the total accessible SSA for the electrolyte ions and are regarded as the E-SSA, which is 1771 m2 g-1 for AC-KOH electrode material as an example.

The capacitance performance of AC-KOH and YP50 was measured through two electrode system (coin-type supercapacitor). Fig. 2 shows the specific capacitance of the capacitors at different current density. In the TEABF4/AN electrolyte system, the specific capacitance of AC-KOH based capacitor is 206, 202 and 198 F g-1 at 0.5, 1 and 2 A g-1, respectively. Accordingly, YP50 based capacitor shows 101, 100 and 100 F g-1 at 0.5, 1 and 2 A g-1, respectively. The galvanostatic charge/discharge curves for AC-KOH based capacitor at current density of 5, 10, 15, 20 and 30 A g-1 are presented in Fig. 3.

The CV curves, galvanostatic charge/discharge curves, rate performances and Nyquist plots of AC-KOH electrode material in 6 M KOH electrolyte are shown in Fig. 4. The CVs (Fig. 4a) were measured in the voltage range of 0−1.0 V at the scan rates of 5, 10 and 20 mV s-1. The galvanostatic charge/discharge curves at different current densities are presented in Fig. 4b. The capacitance of AC-KOH of YP50 at current density of 0.1 A g-1 is 260 and 132 F g-1, respectively. The specific capacitance of AC-KOH is 216 F g-1 at current density of 2 A g-1 (Fig. 4c). The charge transfer resistance and ion diffusion performance were evaluated by the electrochemical impedance spectroscopy (EIS) measurements at a frequency range of 100 kHz to 10 mHz, as shown in Fig. 4d.

The galvanostatic charge/discharge curves for AC-KOH and YP50 based supercapacitors in EMIMBF4 electrolyte system tested at current density of 1 A g-1 are presented in Fig. 5. According to these curves, the capacitance of AC-KOH and YP50 based supercapacitors was calculated, which is 188 and 120 F g-1, respectively. The energy density of AC-KOH device, calculated using the formula Ecell = CpV2/8 (where Cp (F g-1) is the specific capacitance of the device and V (V) is the voltage), is 80 W h kg-1 at power density of 870 W kg-1, and the data of YP50 is 51 W h kg-1 at power density of 870 W kg-1. The power density, P (W kg-1), was calculated according to the formula P = Et (where E (W h kg-1) is the energy density of the device and Δt (s) is the discharge time).

The application of an AC-KOH based coin-type supercapacitor cell for lighting a LED is shown in Fig. 6 and the supplementary video. The coin-type supercapacitor was assembled using AC-KOH as the electrode material and ionic liquid (EMIMBF4) as the electrolyte. The device firstly was charged at 1 A g-1 to 3.5 V and then used to light the LED with a working potential around 2.2 V and working power about 40 mW. The LED could maintain light for ~ 30 minutes.

In addition, the structure and capacitive performance data of AC-KOH material in this work and the comparison data with the reported reports are summarized in Table 3, as shown in below.

Acknowledgements

The authors gratefully acknowledge the financial support from the National Natural Science Foundation of China (NSFC, 51502125), the Natural Science Foundation of Hebei Province of China (Grant E2016408035, B2017408042) and the Research Project of Hebei Education Department of China (BJ2016044).

Footnotes

Transparency document

Supplementary data associated with this article can be found in the online version at 10.1016/j.dib.2018.04.057.

Contributor Information

Yanhong Lu, Email: luyanhong_2003@126.com.

Yongsheng Chen, Email: yschen99@nankai.edu.cn.

Transparency document. Supplementary material

Supplementary material

mmc1.pdf (1.2MB, pdf)

.

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