- Nano Express
- Open Access
Template method synthesis of mesoporous carbon spheres and its applications as supercapacitors
© Wilgosz et al.; licensee Springer. 2012
- Received: 9 January 2012
- Accepted: 17 April 2012
- Published: 29 May 2012
Mesoporous carbon spheres (MCS) have been fabricated from structured mesoporous silica sphere using chemical vapor deposition (CVD) with ethylene as a carbon feedstock. The mesoporous carbon spheres have a high specific surface area of 666.8 m2/g and good electrochemical properties. The mechanism of formation mesoporous carbon spheres (carbon spheres) is investigated. The important thing is a surfactant hexadecyl trimethyl ammonium bromide (CTAB), which accelerates the process of carbon deposition. An additional advantage of this surfactant is an increase the yield of product. These mesoporous carbon spheres, which have good electrochemical properties is suitable for supercapacitors.
- Mesoporous silica
- Carbon spheres
- Mesoporous carbon
Supercapacitors are a fast-developing technology in electric energy storage including lithium-ion secondary batteries, fuel cells, and electrical double-layer capacitors [1, 2]. They are electrochemical storage devices able to fill the gap that exists between batteries and dielectric capacitors from the energy and power density point of view . In recent years electric double layer capacitors (EDLCs) have evoked wide interest, because of their capability to supply high power in short-term pulse, which makes them very good energy storage devices for applications such as hybrid power sources for electrical vehicles, portable electronic devices, and pulse laser techniques . Materials for EDLCs should have a huge surface area to accumulate large amount of charges and size-controllable porous channel system for the easy access to the electrolyte . The most promising materials are carbon spheres because of their commercial availability, price, and abundance . Mesoporous carbon has got remarkable properties such as high specific surface area, large pore volume, low density, thermal conductivity, electrical conductivity, good chemical and mechanical stability, and great application potential to catalysts, electrodes, batteries, sensors, adsorbents in separation processes, gas storage materials, and templates for fabricating nanostructures [7–10]. Mesoporous carbon spheres can be fabricated with the mesoporous silica spheres as the templates . Production of mesoporous carbon spheres, which is an inverse replica templated from mesoporous silica, attracted increasing attention .
In this paper, a simple chemical vapor deposition method for mesoporous carbon spheres (sphere shape) fabrication is presented. This technique is different from the previously reported methods using mesoporous silica spheres [11, 12] because they involve of carbon source being incorporated into the channels of mesoporous structures and subsequent carbonization process. These procedures require additional step to decompose surfactant and subsequent filling carbon into the mesoporous silica. In our case a single CVD process is needed to produce the carbon filled mesoporous silica spheres. These obtained mesoporous carbon spheres show good electrochemical properties in supercapacitors at high current load.
Synthesis of mesoporous silica spheres
m-SiO2 nanospheres were prepared as follows: surfactant hexadecyl trimethyl ammonium bromide (CTAB) (300 mg) was added to a mixture of ethanol (EtOH) (60 ml), distilled water (80 ml) and ammonia (25 wt %, 1,1 mL), then sonicated and subsequent vigorous stirred. After stirring for 30 min. tetraethyl orthosilicate (TEOS) (0,4 ml) was added to the reaction mixture and subsequently stirred at room temperature for 12 h. Finally, the product was obtained through centrifugation and dried.
Synthesis of carbon filled m-SiO2_C
The dried m-SiO2 treated by CTAB was used as a template to prepare the carbon spheres using CVD. This compositon was placed in an alumina boat and set in a tube furnace. Argon and ethylene were introduced at a flow rate of 100 sccm and 30 sccm, respectively. The temperature was raised to 800°C. and the process took 4 h. Afterwards, the resulting m-SiO2_C spheres were thoroughly washed with hydrofluoric acid to remove the silica and obtain the final product.
X-ray diffraction (XRD) was conducted on a Philips diffractometer using Cu Kα radiation. Transmission electron microscopy (TEM) together with Energy Dispersive X-Ray spectrometer as its mode has been utilized to examine the dimensions, structural details and chemical composition of the samples (Tecnai F30 with a field emission gun operating at 200 kV). Raman scattering was conducted on a Renishaw micro Raman spectrometer (λ = 785 nm). The specific surface area was calculated by the Brunauer-Emmett-Teller (BET) metod via Micromeritics ASAP 2010 M instrument. The pore size distribution was determined using the Barret–Joner–Halenda (BJH) method. Thermogravimetric analysis (TGA) was carried out on 10 mg samples using the DTA-Q600 SDT TA Instrument at a heating rate of 10°C/min from room temperature to 900°C under air.
Two-electrode capacitor of diameter 10 mm and mass of 9–10 mg were pressed from a mixture of active material (85%), polyvinylidene fluoride PVDF (10%) and acetylene black (5%). Electrode was composed of the mesoporous carbon spherical spheres and were separated by the glassy fibrous paper and placed between gold current collectors in a teflon Swagelok® type system where 1 mol l–1 H2SO4 solution was an electrolyte. Voltammetry experiments at a scan rate from 1 to 100 m V s -1 and galvanostatic charge/discharge at a current density from 0.2 to 20 A g−1 were used for the estimation of the specific capacitance C expressed in farads (F) per gram of carbon spheres. In this work the results of voltammetry experiments for a better legibility were presented as a function of C = f (E). The VMP3 (Bio-logic Science Instruments, France) multichannel generators were used for the realization of the measurements.
Finally, the HF treatment of the samples resulted in preparation of mesoporous carbon spheres with channels radially oriented with respect to the sphere centre and the mean diameter of 410 nm (Figure 1g, h). It means that the carbon deposited on the spheres surface has been also removed successfully during the acid treatment. EDX spectrum confirm the removal of SiO2 (Figure 1i). To further analyse the final product the Raman spectrum was detected (see inset of Figure 1g). It clearly reveals two the tangential modes i.e. the G mode (1598 cm−1) that is derived from the graphite-like in-plane mode and the disorder induced D band (1300 cm−1). Additionally, TGA of the carbon spheres shown in the inset of Figure 1h indicates that the material starts to decompose in air at 526 0 C. The weight loss increases rapidly with the further increase of the combustion temperature. This process lasts untill all of the carbon spheres were burnt off at about 650°C and at the final stage no ashes were present in the TGA cuvette after the thermal treatment. This clearly indicates the sample quality and the efficiency of silica removal upon HF treatment.
The Brunauer, Emmet, and Teller (BET) method has been used to measure of the surface area of our final product. The total specific surface area of mesoporous carbon spheres is 666.8 m2/g. It can be attributed to the cavity in the carbon spheres. The powder X-ray diffraction (XRD) pattern shows mesoporous silica, mesoporous silica with CVD deposited carbon and mesoporous carbon spheres (Figure 2)b. The sharp peaks at 2.3; 4.18; 4.8; 6.3o in XRD pattern of the starting template (green line) shows the mesoporous silca structure with empty channels. Peaks at 2.8 and 5.7o in XRD spectrum of the sample after CVD (blue line) are assigned to a mesoporous silica filled with carbon, the strongest peak shifted from 2.3 to 2.8o also indicated the blockage of mesoporous channels with carbon. The overlapped peaks at 22 and 24.9o belong to silica and carbon, respectively. The black line corresponding to the XRD of mesoporous carbon spherical spheres exhibits the strong peak at 24.9o ascribed to graphitic carbon, which is corresponding to Raman spectra. However, the peak at 22o disappeared, which means that silica has been completely removed.
Mesoporous carbon spherical spheres were obtained from structured mesoporous silica sphere using chemical vapor deposition (CVD) with ethylene as a carbon feedstock. This procedure does not require additional step to decompose surfactant into carbon. The surface area carbon spheres is large and consists of 666.8 m2/g. The electrochemical properties of the carbon spheres, such as capacity of performance at high current load caused that the carbon nanomaterials could be used for supercapacitor applications.
The work was supported by Foundation for Polish Science within Focus with contract F4/2010, and we are grateful for the revision of the manuscript from the language editor.
- Conway BE: Transition from “Supercapacitor” to “Battery” Behavior in Electrochemical Energy Storage. J Electrochem Soc 1991, 138: 1539–1540. 10.1149/1.2085829View ArticleGoogle Scholar
- Kim H, Fortunato ME, Xu H, Bang JH, Suslick KS: Carbon Microspheres as Supercapacitors. J Phys Chem 2001, 115: 20481–20486.Google Scholar
- Roldan S, Granda M, Menendez R, Santamaria R, Blanco C: Mechanisms of Energy Storage in Carbon-Based Supercapacitors Modified with a Quinoid Redox-Active Electrolyte. J Phys Chem C 2011, 115: 17606–17611. 10.1021/jp205100vView ArticleGoogle Scholar
- Wang K, Wang Y, Wang Y, Hosono E, Zhou H: Mesoporous Carbon Nanofibers for Supercapacitor Application. J Phys Chem C 2009, 113: 1093–1097. 10.1021/jp807463uView ArticleGoogle Scholar
- Liu HY, Wang KP, Teng H: A simplified preparation of mesoporous carbon and the examination of the carbon accessibility for electric double layer formation. Carbon 2005, 43: 559. 10.1016/j.carbon.2004.10.020View ArticleGoogle Scholar
- Xiao T, Heng B, Hu X, Tang Y: In Situ CVD Synthesis of Wrinkled Scale-Like Carbon Arrays on ZnO Template and Their Use to Supercapacitors. J Phys Chem C 2011, 115: 25155–25159. 10.1021/jp208492vView ArticleGoogle Scholar
- Liang C, Li Z, Dai S: Mesoporous Carbon Materials: Synthesis and Modification. Angew Chem Int Ed 2008, 47: 3696–3717. 10.1002/anie.200702046View ArticleGoogle Scholar
- Guo L, Zhang L, Zhang J, Jian Z, Xiangzhi C, Shi J: Hollow mesoporous carbon spheres—an excellent bilirubin adsorbent. Chem Commun 2009, 6071–6073.Google Scholar
- Fang B, Kim M, Yu J: Hollow core/mesoporous shell carbon as a highly efficient catalyst support in direct formic acid fuel cell. Appl Catal 2008, 84: 100–105. 10.1016/j.apcatb.2008.03.005View ArticleGoogle Scholar
- Chai G, Yoon S, Kim J, Yu J: Spherical carbon capsules with hollow macroporous core and mesoporous shell structures as a highly efficient catalyst support in the direct methanol fuel cell. J Chem Commu 2004, 2766–2767.Google Scholar
- Honda H, Kimura H, Sanada Y, Sugawara S, Furuta T: Optical mesophase texture and X-ray diffraction pattern of the early-stage carbonization of pitches. Carbon 1970, 8: 181. 10.1016/0008-6223(70)90112-0View ArticleGoogle Scholar
- Dong A, Ren N, Tang Y, Wang Y, Zhang Y, Hua W, Gao Z: General Synthesis of Mesoporous Spheres of Metal Oxides and Phosphates. J Am Chem Soc 2003, 125: 4976–4977. 10.1021/ja029964bView ArticleGoogle Scholar
- Andreas HA, Conway BE: Examination of the double-layer capacitance of an high specific-area C-cloth electrode as titrated from acidic to alkaline pHs. Electrochim Acta 2006, 51: 6510. 10.1016/j.electacta.2006.04.045View ArticleGoogle Scholar
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