Samira Gharehkhani*a,
Seyed Farid Seyed Shirazi*b,
Siamak Pilban Jahromic,
Mehran Sookhakianc,
Saeid Baradarana,
Hooman Yarmanda,
Azim Ataollahi Oshkoura,
Salim Newaz Kazia and
Wan Jefrey Basirunde
aDepartment of Mechanical Engineering, Faculty of Engineering, University of Malaya, 50603 Kuala Lumpur, Malaysia. E-mail: s_gharahkhani_248@yahoo.com
bDepartment of Mechanical Engineering and Advanced Material Research Center, University of Malaya, 50603, Kuala Lumpur, Malaysia. E-mail: f.shirazi@siswa.um.edu.my; Tel: +60 142646276
cLow Dimensional Materials Research Center, Department of Physics, Faculty of Science, University of Malaya, 50603, Kuala Lumpur, Malaysia
dInstitute of Nanotechnology & Catalysis Research (NanoCat), University of Malaya, 50603 Kuala Lumpur, Malaysia
eDepartment of Chemistry, Faculty of Science, University of Malaya, 50603, Kuala Lumpur, Malaysia
First published on 23rd April 2015
Carbon derived from low cost agricultural waste material was used as a precursor for the preparation of a spongy-like nitrogen doped activated composite from carbon/graphene oxide via a one-step thermal treatment. N-doping and activation of the carbon/graphene oxide mixture were achieved simultaneously by the treatment of urea and potassium hydroxide at 800 °C. The nitrogen content and ratio between the nitrogen species was controlled by the mass ratio of KOH:
carbon. The composite was prepared with a KOH
:
carbon ratio of 1 which resulted in a moderate surface area (1712.4 m2 g−1) and a high nitrogen content (14.51%). The hybrid material gave high specific capacitance (267 F g−1 at 5 mV s−1) and good cycling stability (92.3% capacitance retention after 5000 cycles) in 6 M KOH electrolyte. Hence, the new composite presented in this work can be used as an advanced material for supercapacitor applications.
Based on the reaction mechanism, electrochemical capacitors are categorized into electrical double layer capacitors (EDLCs) and pseudocapacitors.1–3 The materials which are used as EDLCs have acceptable electrical conductivity and good cycle life, but they often suffer from the low specific capacitance. Unlike the first category of electrochemical capacitors (EDLCs), pseudocapacitors have good specific capacitance due to the Faradaic reactions, although the lower electrical conductivity and cycling stability would limit their applications.4 With regards to the advantages and disadvantages of both categories of electrochemical capacitors, it can be concluded that the introduction of materials with higher specific capacitance, cycle life and electrical conductivity could lead to wider applications of such materials.
Among the different types of electrode materials, such as conductive polymers,5 graphene6 and carbon nanotubes,7–9 the carbons with high surface area (activated carbon (AC)) have been used commercially for EDLC applications.10,11 Fossil-fuel based precursors, and biomass materials can be used to prepare the AC.12–16 Compared to the fossil-fuel materials, these biomass precursors are cheaper and environmental friendly. Oil palm empty fruit bunch (EFB), a non-wood fiber17 is a suitable biomass precursor for the preparation of AC. EFB is the primary solid waste of palm oil mill processing and is abundant in south east Asia. The annual production of crop residue in the oil palm mills is estimated around 33 million tons in the form of EFB, fiber and shell. Hence, the lignocellulosic EFB is a low-cost and commercially available material for the production of carbonaceous substances.18
AC can be produced by either physical or chemical activation process. In the physical activation process, an activation gas e.g., CO2, steam or mixture of gases is used to prepare the activated carbon. In the chemical activation process, the carbon precursor are mixed with chemical reagents such as ZnCl2, H3PO4, NaOH and KOH.19 The use of KOH in the activation process was reported previously.14,15,20 Compared to other reagents such as ZnCl2, KOH is more eco-friendly, therefore is more preferred in the chemical activation process.21
Capacity improvement of porous carbons is one of the main focus areas in electrochemical studies.22 Recently, different approaches such as the synthesis of a high surface area carbon using a composite containing carbon and graphene, has been reported.23,24 Graphene, a 2D single layer of sp2 carbon atoms, exhibits very high electrical conductivity.25 Many studies have been reported on the electrochemical properties and capacitor performances of different types of graphene with a variety of chemical and morphological structures such as graphene oxide (GO), graphene nanoplatelet and reduced graphene oxide (RGO).26–30 The different methods for the reduction of GO includes the use of chemicals such as hydrazine hydrate, or reduction via high temperature thermal treatment have been reported.6,31,32 Although graphene based compounds are excellent materials for capacitor applications, the synthesis of graphene in large batch is difficult and expensive. Moreover, the limited surface area of graphene despite its high theoretical surface area (2630 m2 g−1) is another disadvantage. By considering these facts, it could be conceived that the use of graphene as a guest material in an amorphous carbon could be more efficient and augments the electrical conductivity and charge-carrier mobility of the composite.
Another alternative strategy is to improve the capacitance of the carbon materials by doping the carbon networks with heteroatoms such as nitrogen and oxygen, which can improve the charge transfer along the carbon network.33–35 Moreover, the surface groups on the carbon materials may induce an acid–base property, which could improve the capacitance of the carbon materials through the pseudocapacitance reactions.36,37 The incorporation of nitrogen atoms into a carbon network has been accomplished by treatment methods using ammonia or urea,38 or in situ doping methods using nitrogen source precursors such as melamine resin,39 polyvinylpyridine,40 polypyrrole,41 polyaniline42 and chitosan.43 Zhao, et al.44 synthesized porous nitrogen doped composite via co-pyrolysis of lignosulfonate and GO. Urea was used as the nitrogen source and the nanoporous structure with a nitrogen content of 7.41% gave high capacitance value with 92.5% capacitance retention after 1000 cycles.
It is more worthwhile to synthesize materials with high capacitance from renewable sources, with a facile single-step and scalable synthetic process. Therefore, in this report, for the first time, we introduce a spongy-like structured composite containing a carbon derived from agricultural waste materials and GO which was synthesized via the simultaneous nitrogen doping and activation process for supercapacitor electrodes. This green, low cost, facile and effective single-step approach was employed to prepare a nitrogen doped activated carbon/RGO composite which has bright prospect as an extraordinary material for electrochemical applications.
To study the effect of GO and nitrogen doping on the sample properties, three series of undoped samples with and without GO and impregnated only with the KOH (denoted as AC, A-CRGO-1 and A-CRGO-4) were prepared as the control samples. The AC sample was prepared with a KOH:
C ratio of 4. Moreover GO was thermally reduced to RGO during the process, hence a thermally reduced graphene oxide (RGO) sample was prepared from the heating of GO (without agents) in the furnace, with the same procedure.
The specific capacitance of the electrodes were calculated from the CV curves using eqn (1) where Cs is the specific capacitance of the sample (F g−1), v is the scan rate (V s−1), m is the mass of active material (g), ΔVif is the applied potential window, and the integral term is equal to the area under the CV curve.
![]() | (1) |
The activation process with higher amount of KOH leads to a larger exposition of the amorphous structure of carbon, which is due to the amount of gases produced during the activation process by KOH. Fig. 2c and d show that the simultaneous N doping and activation process produced more wrinkles to the structure as compared to activation process (Fig. S1a and b†). However an increase in mass ratio of KOH:
carbon leads to a higher porosity and surface roughness. On the other hand, N doping introduces more wrinkles to the surface. The distribution of the nitrogen atoms in NA-CRGO-1 structure was further characterized by FESEM elemental mapping (Fig. 2e). The homogeneous distribution of the nitrogen atoms shows that nitrogen can be properly doped in the composites. However, it seems that there is a slight difference between the amounts of N doped atoms into the composite components. The energy dispersive X-ray (EDX) data for NA-CRGO-1 (Fig. S2†) demonstrated that RGO (zone 1) in the composite probably has more affinity to accept foreign atoms than carbon (zone 2).
![]() | ||
Fig. 2 (a–d) TEM images of the AC, RGO, NA-CRGO-1 and NA-CRGO-4 respectively. (e) FESEM elemental mapping of NA-CRGO-1. |
The nitrogen adsorption/desorption isotherm and pore size distributions of the N-doped samples, are presented in Fig. 3a and b respectively. The isotherms in Fig. 3a show type I curve, based on the International Union of Pure and Applied Chemistry (IUPAC), which presents a microporous structure with small amount of mesoporous appearance for the NA-CRGO-1 and NA-CRGO-4. Fig. 3b presents the pore size distribution curves which show that the NA-CRGO-4 has higher pore volume than NA-CRGO-1 due to the ratio of the KOH:
C. The pore size of the samples is basically less than 2 nm. Besides the micropores, the contribution of meso scale pores with size more than 2 nm, can be seen in the micro-graphs which could facilitate the transportation of the electrolyte ions.45,46 The estimated surface areas based on the Brunauer–Emmett–Teller (BET) method and pore structure characterization data for N-doped samples are presented in Table 1. The estimated BET specific surface areas are 1712.4 and 2261.2 m2 g−1 for NA-CRGO-1 and NA-CRGO-4, respectively, which demonstrates an ultrahigh surface area compared to the untreated carbon (7.5 m2 g−1). The BET surface area of GO reported in the literatures is less than 100 m2 g−1.47,48 Moreover, the micropore to mesopore volume ratio has decreased from 2.87 for NA-CRGO-1 to 1.83 for NA-CRGO-4, respectively.
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Fig. 3 (a) N2 adsorption and desorption isotherms and (b) pore size distribution of N doped samples. (c) The Raman spectra of samples. |
Sample | SBET (m2 g−1) | Total pore volume (cm3 g−1) | Micropore volume (cm3 g−1) | Mesopore volume (cm3 g−1) |
---|---|---|---|---|
NA-CRGO-1 | 1712.4 | 0.93 | 0.69 | 0.24 |
NA-CRGO-4 | 2261.2 | 1.31 | 0.84 | 0.46 |
Generally, the use of KOH for the preparation of activated carbon yields a carbon structure with high surface area, high microporous structure and a narrow pore size distribution. To describe the mechanism of activation with KOH, it was proposed that the alkali metal intercalates in the carbon lattice and acts as an electron donor which promotes the reaction during gasification.21,49 The reaction between KOH and carbon can be described in the following reaction:50,51
6KOH + 2C ↔ 2K + 3H2 + 2K2CO3 | (2) |
When the activation temperature is higher than 700 °C, the following reactions may occur52
K2CO3 → K2O + CO2 | (3) |
K2CO3 → 2C + 2K2O | (4) |
K2O + C → 2K + CO | (5) |
Raman spectroscopy is a powerful tool for the investigation of structural changes of carbon materials. The peak intensity of the D and G bands in the Raman spectra are shown in Fig. 3c. The Raman spectra of the prepared samples show the D-band at ∼1340 cm−1 and the G-band at ∼1598 cm−1. Compared with A-CRGO-1 and A-CRGO-4, the G peak of NA-CRGO-1 and NA-CRGO-4 exhibit a slight blue shift. One of the most important parameters in the Raman spectrum is the peak intensity ratio of the D and G bands, (ID/IG) which is attributed to the disordered crystal structures of the carbon material. The ID/IG values for NA-CRGO-4, NA-CRGO-1, A-CRGO-4, A-CRGO-1 and AC, are 0.73, 0.61, 0.51, 0.42 and 0.36, respectively. It is noted that an increase in the ID/IG in the NA-CRGO samples prepared from the combination of N-doping and activation processes lead to a less degree of graphitization which probably resulted from the incorporation of N atoms.53 Moreover, the Raman spectra of GO and RGO are presented in Fig. S3.† The ID/IG values of GO and RGO are 0.60 and 0.95, respectively. The increase of the ID/IG of RGO compared to GO confirms the reduction of GO to RGO.54,55
Table 2 presents the chemical composition of the samples, from the XPS data. Moreover the total carbon, hydrogen, oxygen and nitrogen contents (%) in AC, A-CRGO and NA-CRGO samples obtained by the elemental analysis (CHN) method was utilized in initial analysis of the samples (Table S1†).
Sample | C (atom%) | O (atom%) | N (atom%) | N1 | N2 | N3 | N/C |
---|---|---|---|---|---|---|---|
AC | 59.65 | 40.35 | — | — | — | — | — |
A-CRGO-1 | 79.02 | 20.98 | — | — | — | — | — |
A-CRGO-4 | 65.50 | 34.50 | — | — | — | — | — |
NA-CRGO-1 | 68.95 | 16.54 | 14.51 | 5.29 | 5.85 | 3.36 | 0.21 |
NA-CRGO-4 | 74.09 | 14.38 | 11.53 | 4.85 | 5.08 | 1.60 | 0.15 |
The difference between the CHN and XPS results is due to the fact that CHN determines the bulk composition of each elements, while XPS presents the surface composition of the elements.37 In order to reveal the elemental composition of the surface clearly, the resulting XPS spectra are displayed in Fig. 4. As shown in Fig. 4a, the N 1s peak is only present in the NA-CRGO samples, but not in the A-CRGO and AC samples. The N 1s peak in the nitrogen doped samples (NA-CRGO-1 and NA-CRGO-4) was deconvoluted into three different regions. The three nitrogen functional groups (Fig. 4b and c) are pyridinic-N (N1, ∼398 eV), pyrrolic-N (N2, ∼400 eV) and quaternary-N (N3, ∼401 eV). As listed in Table 2, the NA-CRGO-1 consists more nitrogen atoms as well as higher N:
C ratio compared to NA-CRGO-4, which shows the possibility of the increase of N content by decreasing the KOH dosage.34,56 The dominant sites in both N doped samples are pyridinic nitrogen and pyrrolic nitrogen and NA-CRGO-1 shows a proper ratio of nitrogen species with more quaternary nitrogen atoms. Fig. 4d and e present the C 1s core level peak of the NA-CRGO-1 and NA-CRGO-4 respectively. The main peak at 284.5 eV corresponds to C
C. The three small peaks located at 285.50, 287.08 and 288.38 eV; and 285.42, 286.68 and 287.98 eV in the NA-CRGO-1 and NA-CRGO-4 spectra respectively, are ascribed to C
N & C–O, C–N & C
O and O–C
O. Although the peaks at around 285 and 287 eV are usually assigned to the C–O and C
O respectively, this peak could be attributed to the C
N and C–N in the nitrogen doped samples.57 In addition, Table 2 reveals a lower oxygen content in the NA-CRGO samples compared to the A-CRGO samples. The O 1s peaks of NA-CRGO-1 and NA-CRGO-4 (Fig. S4†) can be deconvoluted into the C
O, C–OH & C–O–C and COOH carboxylic groups and water.47 A schematic structure of the nitrogen surface functional groups on carbon is shown in Fig. 4f.
The CV profiles and the relation between the specific capacitance and scan rate for the NA-CRGO-1 and NA-CRGO-4 are shown in Fig. 5b–d. The same trend can be observed in the NA-CRGO samples. The decrease of specific capacitance for NA-CRGO-1 at scan rate 5 mV s−1 to 20 mV s−1 is more profound compared to the scan rate from 20 mV s−1 to 100 mV s−1 which can be attributed to a higher contribution of the pseudocapacitance behavior in lower scan rates (Fig. 5d).
The specific capacitance for NA-CRGO-1 is comparable with the reported N-doped porous carbons,44 which is probably due to the proper structure of the material which can increase the electrolyte penetration and facilitate the transport of electrons in the active material, and an appropriate ratio of edge nitrogen atoms (N1 and N2) to N3.60
Fig. 6a and b show the galvanostatic charge–discharge curves for all samples at 0.3 A g−1, and NA-CRGO-1 at different current densities respectively. The specific capacitance calculated from the galvanostatic discharge curves at 0.3 A g−1 are 214, 175, 86, 99, 80 and 25 F g−1 for NA-CRGO-1, NA-CRGO-4, A-CRGO-1, A-CRGO-4, AC and RGO respectively.
The EIS test was performed to further investigate the electrochemical behavior of the N-doped samples. The Nyquist plots show a semicircle at higher frequency region and a straight line at lower frequency region for the samples (Fig. 6c). The characteristic impedance plots for AC and RGO are also presented in Fig. 6c. The NA-CRGO-1 has a larger slope compared to NA-CRGO-4, which confirms its ideal capacitive behavior.27,57 Furthermore, the diameter of the semicircle is an indication of the charge transfer resistance and electrode conductivity.61 The NA-CRGO-1 shows a smaller semicircle diameter compared to NA-CRGO-4. It can be concluded that NA-CRGO-1 has lower charge transfer resistance, which is due to the higher amount of quaternary-N atoms. Moreover, the NA-CRGO-4 possesses a smaller semicircle than AC, affirming that the presence of RGO can increase the electrode conductivity.62 The cycling stability, another important measurement in the capacitor studies, was investigated by repeating the CV test in a potential range of −1 to 0 V at a scan rate of 70 mV s−1. The NA-CRGO-1 shows a good capacitance retention ratio after 5000 cycles (Fig. 6d), with only 7.7% decrease in the capacitance after 5000 cycles, which indicates an excellent cycling performance of the NA-CRGO-1 without any loss of the active material from the substrate.
Footnote |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra01525a |
This journal is © The Royal Society of Chemistry 2015 |