Low-cost and high energy density asymmetric supercapacitors based on polyaniline nanotubes and MoO 3 nanobelts

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Electronic Supplementary Material (ESI) for Journal of Materials Chemistry A. This journal is The Royal Society of Chemistry 2014 Electronic Supplementary Information Low-cost and high energy density asymmetric supercapacitors based on polyaniline nanotubes and MoO 3 nanobelts Hui Peng, a Guofu Ma,* a Jingjing Mu, a Kanjun Sun, b Ziqiang Lei* a a Key Laboratory of Eco-Environment-Related Polymer Materials of Ministry of Education, Key Laboratory of Polymer Materials of Gansu Province, College of Chemistry and Chemical Engineering, Northwest Normal University, Lanzhou 730070, China b College of Chemistry and Environmental Science, Lanzhou City University, Lanzhou 730070, China *Corresponding authors. E-mail: magf@nwnu.edu.cn; Leizq@nwnu.edu.cn Experimental details Materials: Aniline monomer (AN, Shanghai Chemical Works, China) was distilled under reduced pressure. D-tartaric acid (D-TA, Shanghai Chemical Works, China), ammonium persulfate (APS, Tianjin Damao Chemical Co., China) and sodium molybdate (Na 2 MoO 4 2H 2 O, Tianjing Chemical Co., China), solutions were prepared using deionized water. All other chemical reagents were in analytical grade. Synthesis of PANI nanotubes: The PANI nanotubes were fabricated similar to our previous reported literature. [S1] In a typical process, aniline monomer (2 mmol) and D-tartaric acid (1 mmol) were dissolved in 10 ml of deionized water with magnetic stirring for 20 min at room temperature. After that, the resulting solution was cooled to 0-5 o C in an ice bath and an aqueous solution of ammonium persulfate (2 mmol in 5 ml of deionized water) cooled in advance was added drop-bydrop into the above solution. The reaction was carried out with magnetic stirring below 5 o C for 10 h. The resulting precipitate was washed several times with deionized water and ethanol, respectively. Finally, the product was dried at 60 o C for 12 h to obtain a dark green powder. Synthesis of MoO 3 nanobelts: In a typical process, 4.84 g Na 2 MoO 4 2H 2 O was dissolved in 10 ml S1

deionized water. Then 16 ml 4 M HClO 4 was added dropwise to the molybdate solution under constant stirring. Finally, this solution was transferred into a 100 ml Teflon-lined stainless steel autoclave and heated at 140 o C for 24 h. After cooled to room temperature naturally, the resulting precipitates of MoO 3 were collected by filtration, washed with distilled water and absolute ethanol for several times to remove the residue of reactants, and then dried in vacuum at 60 o C for 12 h. Materials Characterization The morphologies of the as-prepared products were examined with field emission scanning electron microscopy (FE-SEM, JSM-6701F Japan) at an accelerating voltage of 5.0 kv. The structure of the PANI samples was characterized by a transmission electron microscopy (TEM, JEM-2010 Japan). X-ray diffraction (XRD) of samples was performed on a diffractometer (D/Max-2400, Rigaku) advance instrument using Cu Kα radiation (k =1.5418 Å) at 40 kv, 100 ma. The 2θ range used in the measurements was from 5 to 80. Three-electrode fabrication For conventional three-electrode system, the glassy carbon electrode with a diameter of 5 mm was used as the working electrode. The working electrodes were fabricated similar to the literature. [S2] Typically, 4 mg of electrode material was ultrasonically dispersed in 0.4 ml of 0.25 wt% Nafion (DuPont, USA). The above suspension of 8 μl using a pipet gun was dropped onto the glassy carbon electrode and dried at room temperature. The three-electrode system was test in 1 M H 2 SO 4 aqueous solutions, platinum electrode serves as the counter electrode, and standard calomel electrode (SCE) as the reference electrode, respectively. Two-electrode cell fabrication The capacitive performance of asymmetric supercapacitors was investigated using a twoelectrode testing cell. The working electrode was prepared by mixing the electroactive material with polyvinylidene fluoride (PVDF) and commercial carbon black (8:1:1) in N-methyl-2- pyrrolidone (NMP) until homogeneous slurry. The slurry was coated on carbon plate (99.99%, 3 mm) with a working area of 1.0 cm 2 and the electrodes were dried at 120 o C for 12 h. To construct an ASC, the loading mass ratio of active materials (PANI//MoO 3 ) was estimated to be 0.89 from S2

the specific capacitance calculated from their galvanostatic charge/discharge curves. The PANI positive electrode and MoO 3 negative electrode were pressed together and separated by a thin polypropylene film. The electrochemical measurements of the ASCs were carried out in a two electrode cell at room temperature in1 M H 2 SO 4 electrolyte. Electrochemical measurements The electrochemical properties of the samples were investigated by cyclic voltammetry (CV) and galvanostatic charge/discharge measurements in three-electrode cell and two-electrode configuration using a CHI 660D electrochemical workstation. The cycle-life stability was performed using computer controlled cycling equipment (LAND CT2001A, Wuhan China). Electrochemical impedance spectroscopy (EIS) measurements were performed with the Autolab PGSTAT 128N equipped (Eco-chemie, Netherland) with FRA module, the frequency ranging from 10 mhz to 100 khz and an impedance amplitude of ±5 mv at open circuit potential. The gravimetric capacitance from galvanostatic charge/discharge was calculated by using the formula of C s =4IΔt/(mΔV) for the two-electrode cells, while, C s* =IΔt/(mΔV) for the threeelectrode system, where I is the constant current (A) and m is the mass (g) of electrode material (For the two-electrode cells, m is the total mass of positive and negative electrodes), Δt the discharge time and ΔV the voltage change during the discharge process. The specific energy density (E, Wh kg -1 ) and power density (P, W kg -1 ) for a supercapacitor cell can be calculated using the following equations: E=1/2CV 2 and P=E/t, where C is the specific capacitance of supercapacitor cell, V is voltage change during the discharge process after IR drop in V-t curve, and t is the discharge time. S3

Figure S1. Nyquist plots of PANI and MoO 3 electrodes for three-electrode system and its expanded high frequency region (inset). Figure S2. Comparative CV curves of PANI and MoO 3 electrodes performed in three electrode cell in 1 M H 2 SO 4 electrolyte at a scan rate of 100 mv s -1 S4

Figure S3. Nyquist plots of PANI//MoO 3 asymmetric supercapacitors for two-electrode system (the inset of modeled equivalent circuit of electrochemical impedance spectroscopy). S5

Table S1. Performances comparison of ASCs with positive and negative electrodes ASCs structure Electrolyte Operation voltage (V) Energy density (Wh kg -1 ) Power density (W kg -1 ) Ref. GrMnO 2 //GrMoO 3 Na 2 SO 4 2.0 42.6 276 [S3] CNT/MnO 2 //CNT/In 2 O 3 Na 2 SO 4 2.0 25.5 50.3K [S4] RGO-RuO 2 //RGO-PANI KOH 1.4 26.3 150 [S5] MnOOH@RGO//AC KOH 1.6 41.1 400 [S6] Ni(OH) 2 /UGF//a-MEGO KOH 1.8 13.4 85K [S7] CoO@PPy//AC NaOH 1.8 43.5 87.5 [S8] Ni(OH) 2 /graphene// porous graphene Ni(OH) 2 /graphene// RuO 2 /graphene KOH 1.6 77.8 174.7 [S9] KOH 1.5 48.0 230 [S10] MnO 2 //CNT Na 2 SO 4 2.0 47.4 200 [S11] MnO 2 //FeOOH Li 2 SO 4 1.85 24.0 450 [S12] NiCo 2 O 4 @MnO 2 NaOH 1.5 35.0 163 [S13] PbO 2 //AC H 2 SO 4 1.8 31.6 201 [S14] Ni-Zn-Co oxide/hydroxide// Porous carbon Na 2 SO 4 1.5 41.6 100 [S15] PANI//MoO 3 H 2 SO 4 2.0 71.9 254 Present S6

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