Carbon Letters Vol. 8, No. 4 December 2007 pp. 285-291 Carbon Material from Natural Sources as an Anode in Lithium Secondary Battery Sunil Bhardwaj ♠, Maheshwar Sharon , T. Ishihara , Sandesh Jayabhaye , Rakesh Afre , T. Soga and Madhuri Sharon 1, 1 3 3 2 1 4 1 Nanotechnology Research Center, Birla College, Kalyan 421304, Maharashtra, India Department of Applied Chemistry, Faculty of Engineering, Oita University, Oita 870-1192, Japan 3 Graduate School of Engineering, Nagoya Institute of Technology, Nagoya. Japan 4 Monad Nanotech Private Ltd., A702, Bhawani Towers, Adishankaracharya Marg, Powai, Mumbai - 400 076, India ♠e-mail: [email protected] (Received June 14, 2007; Accepted October 24, 2007) 2 Abstract Carbon materials of various morphologies were synthesized by pyrolysis of Soap-nut seeds (Sapindus mukorossi), Jack Fruit seeds (Artocarpus heterophyllus), Date-seeds (Phoenix dactylifera), Neem seeds (Azadirachta indica), Tea leaves (Ehretia microphylla), Bamboo stem (Bambusa bambus) and Coconut fiber (Cocos nucifera), without using any catalyst. Carbon materials thus formed were characterized by SEM XRD and Raman. Carbon thus synthesized varied in size (in µm) but all showed highly porous morphology. These carbon materials were utilized as the anode in Lithium secondary battery. Amongst the various precursors, carbon fibers obtained from Soap-nut seeds (Sapindus mukorossi) and Bamboo stem (Bambusa bambus), even after 100th cycles, showed the highest capacity of 130.29 mAh/g and 92.74 mAh/g respectively. Morphology, surface areas and porosity of carbon materials obtained from these precursors were analyzed to provide interpretation for their capacity to intercalate lithium. From the Raman studies it is concluded that graphitic nature of carbon materials assist in the intercalation of lithium. Size of cavity (or pore size of channels type structure) present in carbon materials were found to facilitate the intercalation of lithium. Keywords : Carbon materials, Lithium battery carbon, Lithium intercalation, carbon from oil seeds, carbon from fibrous plant 1. Introduction The application of lithium battery as a portable energy source is increasing very fast [1] especially because it can provide as high as 3 V cell potential. Moreover, cost of electrode is another consideration which needs to be lowered by developing cheaper materials. Lithium metal as anode, in conjunction with an organic electrolyte results in nonuniform formation of a passive film on the anode surface [24] causing dendrite growth of lithium metal. Lithium alloys e.g. LiSn becomes very large during insertion/deinsertion of lithium [5]. Hence, scientists are looking for some other material like graphite etc which could be used as an anode in aqueous solution. It has been observed that electrochemical intercalation of lithium in graphite [6] generates considerable negative potential close to that of lithium and is less reactive and easily reversible. Therefore, graphite like materials are expected to facilitate intercalation and deintercalation in lithium battery (Fig. 1). Because they can either accept or donate electrons. As a result various attempts have been made to use carbon nanotubes (CNT) as the anode in lithium ion battery [3,7-9]. The intercalation of Li-ion with carbon depends upon various factors such as pore size (either the size of the diameter of the CNT or pore size of channels present in fibrous carbon materials), density, surface area, and activation of CNM etc [10]. The capacity of graphitized carbon is theoretically calculated to be 372 mAh/g (LiC6). One of the major disadvantage with carbon nanotubes in comparison with either graphite or coke as a raw material is the high cost of production [11]. Carbon nanomaterials have been synthesized mainly from precursors which are derived from either fossil materials or petroleum based products. These fossil materials are destined to deplete. Therefore, search for precursors which are derived from plants especially the waste part or non-edible part of plants was thought of. Sharon et al. [12] have been making efforts to find out suitable plant derived precursors to synthesize carbon nano-materials. They have also [3, 1316] studied the intercalation of lithium with carbon nanobeads synthesized from camphor. As an extension of their work, precursors from various other plant based materials like oil seeds, fibrous stems like baggas, cotton etc. were selected to synthesize carbon materials and examine whether they could give better results than what was obtained with 286 Sunil Bhardwaj et al. / Carbon Letters Vol. 8, No. 4 (2007) 285-291 A schematic diagram to show how the intercalation takes place in the host lattice (e.g. graphite) and charging/discharging process in lithium battery. Fig. 1. Schematic diagram showing the apparatus for the preparation of carbon materials by pyrolysis of natural precursors. Fig. 2. carbon nano beads prepared from camphor. We have examined 30 different plant based precursors for this purpose, but in this paper, we report the result of lithium intercalation by carbon materials obtained from the pyrolysis of some selected oil seeds and stems: Soap-nut seeds (Sapindus mukorossi), Jack Fruit seeds (Artocarpus heterophyllus), Date-seeds (Phoenix dactylifera ), Neem seeds (Azadirachta indica), Tea leaves (ehretia microphylla), Bamboo stem (Bambusa bambus) and Coconut fiber (Cocos nucifera), because carbon materials obtained from these precursors showed better capacity for Lithium intercalation, as compared to results obtained with other precursors. 2. Experimental: 2.1. Preparation of Carbon Soap-nut seeds (Sapindus mukorossi), Jack Fruit seeds (Artocarpus heterophyllus), Date-seeds (Phoenix dactylifera ), Neem seeds (Azadirachta indica), Tea leaves (ehretia microphylla), Bamboo stem (Bambusa bambus) and Coconut fiber (Cocos nucifera) were washed with water and dried in oven for three hours at 100oC. Known weight of precursor was kept in a quartz boat and inserted into a quartz tube kept in the furnace (Fig. 2). Furnace was thoroughly closed and flushed with Nitrogen gas for 15 min to flush out the air from the quartz tube. Through out the pyrolysis as well as during cooling the furnace, the flow of Nitrogen was maintained at 50 cc/min. The furnace was heated to 850oC and maintained at that SEM micrographs of carbon materials obtained by the pyrolysis of various plant based precursors. Fig. 3. temperature for 3 h to complete the process of pyrolysis. After cooling the furnace, carbon material was taken out and powdered using motor pestle and were weighed to find out the % yield. Carbon was then purified by soaking in 3M HNO3 for 3 h followed by several washes with distilled water and finally dried at 100oC. Purified carbon materials were characterized and used as anode in lithium battery. 2.2. SEM characterization SEM (FEI quanta 200) of carbon materials obtained by the pyrolysis was examined (Fig. 3). SEM micrograph showed presence of pores and cavity. The size of cavity or pore size of channels present in carbon materials was also calculated from SEM micrographs (Table 1). SEM micrograph of carbon from Tea leaves appears like bee hives filled with small pebbles of about 1 µm diameter. The magnified view of SEM micrograph suggests that each pebble is made of clusters of carbon nano beads of about Carbon Material from Natural Sources as an Anode in Lithium Secondary Battery 287 IG/ID Ratio, Pore Size and Surface Area Obtained with Carbon Materials Obtained from Various Precursors Pore size Surface Area Carbon material obtained Capacity (mAh/g) IG/ID ratio (µm) (m2/g) From following plant’s precursors after 100th Tea (Ehretia microphylla) 133.76 0.999 1.25 96.21 Coconut fiber (Cocos nucifera) 137.5 1.007 5-9 55.59 Bamboo(Bambusa bambus) 192.74 1.025 8.15 49.17 Soap-nut seed (Sapindus mukorossi), 130.29 1.025 8.25 114.03 Jack fruit seed (Artocarpus heterophyllus) 115.90 0.998 114.05 Date-seed (Phoenix dactylifera) 115.31 0.990 18.25 29.22 Neem seed (Azadirachta indica) 110.71 0.998 12.25 14.25 Table 1. 500 nm diameter. Carbon from coconut fiber is heavily porous in nature and appears like a strainer. The pores of carbon have varying sizes ranging from 5-9 µm diameter. Carbon from bamboo has structure composed of bundles of channels lined together of approximately 10 µm diameter. Soap-nut seeds yielded porous carbon block which looked like cotton balls. It had disorganized pores all over the surface. Size of pores is around 8 µm diameter. Carbon fibers obtained from jack fruit seed also has cotton ball like appearance with disorganized pores all over on the surface having similar pore size as that of the soap-nut carbon. Carbon from date-seeds is like fossilized porous rock with large pores (18.25 µm). Carbon from neem seed appears like rectangular block with some cavities on the surface. Details of the pore sizes of these carbon materials, as calculated from the SEM micrograph are given in Table 1. 2.3. Surface area measurement Adsorption of methylene blue in liquid phase by natural solids: activated carbon, charcoal, graphite, and silica for specific surface area determination has been widely adopted [17, 18]. In absence of BET surface area measurement unit, it was decided to measure the surface area by methylene blue technique. Various concentrations (ranging from 0.1 × 10− 5 to 1 × 10− 5 M) of Methylene blue (Lobe Chemie) were prepared in distilled water and their absorbance at its λmax (670 nm) were recorded with a spectrophotometer (Systronic Double Beam Spectrophotometer 2203). These optical densities were plotted against concentration of methylene blue. This graph was used as the standard graph for the calculation of methylene blue present in the measuring samples. The molar extinction coefficient was calculated which lies in the range of (3.9 − 9.5) × 10− 4. This is similar to the reported value by Bergman and O’Konski [17]. 0.025 g of carbon powder was added to 30 cc of methylene blue solution of known concentration (5 × 10− 5 M). The mixture was stirred until the carbon got submerged in the dye solution. This mixture was kept at room temperature for 24 h and shaken periodically. The optical density of the supernatant liquid was determined. The concentration of methylene blue adsorbed by the carbon nanomaterial was calculated from the difference between the methylene blue concentration before and after adsorption onto the carbon by using the standard graph. From this difference in concentration of Methylene blue the surface area of carbon was calculated by using equation-1. (1) S(surface area, km2/kg) = NgaMBN10− 20/M where Ng, aMB, N and M are number of molecule of methylene blue adsorbed at the surface of carbon (i.e., Ng = Nm * M), surface area of one molecule of methylene blue (which is 197.2 Å2), Avagador’s number (6.02 × 1023 mole− 1) and molecular weight of methylene blue (373.9 g mol− 1) respectively. Nm is the number of moles of methylene blue per gram of carbon required to form a monolayer. 10− 20 is the conversion factor to get km2/kg. Results of the surface area of carbon materials are shown in table-1. Surface area calculated with methylene blue may not be as accurate as the BET measurement, because the adsorption of methylene blue over the carbon material may be due to either of the scheme as shown in Fig. 4. If shape of the methylene blue is like cylindrical type, surface area will depend upon the orientation of methylene molecule with A schematic description of possibilities of methylene blue adsorbing on the carbon materials. If methylene molecule takes the shape of cylindrical type, then it can get adsorbed by either attaching as A or B. If spherical then it has one possibility as C. Fig. 4. 288 Sunil Bhardwaj et al. / Carbon Letters Vol. 8, No. 4 (2007) 285-291 Raman spectra of carbon materials prepared from various plant based precursors showing their relative intensities for G- and D-bands. Fig. 5. carbon materials. If adsorbed like “A” (Fig. 4) then the calculated surface area will be larger than if it is adsorbed as “B”. However if it is spherical “C”, then it will give more or less same result as one would obtain with BET technique. Assuming the molecule of methylene blue to be spherical, Chongrak Kaewprasit et al [18] observed that the surface area of cotton fiber calculated by methylene blue technique was 32 times more than what observed with BET measurements. Whether the same result would be obtained with carbon fiber needs to be checked. Results of surface area (table-1) suggest that surface area of carbon material is highest for carbon material obtained from Jackfruit seed (114.05 m2/g) and Soap-nut seed (114 03 m2/g). 2.4. Raman spectroscopic studies Raman spectra (JASCO, NRS-2100) of each carbon materials were taken and the results are shown in Fig. 5. Raman spectra of all compounds show intense peaks for D- and G- bands. It appears that D- band and G-bands for all carbon materials measured have shifted more towards higher wave number as compared to spectra of diamond or graphite (not shown in figure). The IG/ID ratio of carbon materials (Table 1) obtained from Soap-nut seed and Bamboo fiber show highest value suggesting that it contains more graphitic carbon than disordered carbon atoms. Intensities of Raman spectra observed with carbon materials obtained from these precursors follows: Date seed > Soap-nut seed > Coconut fiber > Bamboo stem > Neem seed > Tea leaves > Jackfruit seed. It is interesting to note that peak heights of G and D bands for carbon obtained with Soap-nut seed, Coconut fiber and Date seeds are higher than other carbon materials and amongst these three, carbon from Date seed shows maximum peak height (Fig. 5). 2.5. XRD studies of carbon nanomaterials XRD of carbon materials synthesized from Tea leaves, Soap-nut seeds, Jackfruit seed and Neem seeds are shown in figure 6. XRD spectrum shows the presence of (002) and (100) plane of graphite. Carbon derived Soap-nut seed showed sharpest peak suggesting that they are more crystalline compared to carbon materials obtained from Tea leaves and Neem seed. XRD of carbon from Jack fruit seed suggested presence of some amorphous carbon also. Whereas XRD of carbon from Coconut fiber, Date-seeds, Bamboo stems (not shown here), showed no peaks and even the intensities of spectrum was also very less. 2.6. Electrochemical measurements Each purified carbon sample was mixed with ethylene- XRD of carbon nanomaterials synthesized by pyrolysis of different plant based precursors: Tea leaves, Ritha, Jackfruit and Neem seed. Fig. 6. Carbon Material from Natural Sources as an Anode in Lithium Secondary Battery 289 First Charging (A) and discharging (B) curve obtained with carbon nanomaterials obtained from different plant based precursors. Fig. 7. propylene dimethyl-monomer (EPDM) in cyclohexane and then pressed into a stainless-steel grid on the stainless-steel plate as an anode. A constant dc current was applied across the anode and a Li-metal counter electrode to measure the extent of Li-intercalation capacity of the anode. Ethylene carbonate (EC): dimethyl carbonate DMQ (1 : 20 solution), dissolved in LiPF6 (1 wt. %), were used as an electrolyte. The charge-discharge characteristics were measured between 0 and 1.5 V (Fig. 7). The results of charging/discharging with 100 cycles are shown in Fig. 8. From the results of charging/discharging curves (Fig. 8), it appears that the highest capacity of 850 mAh/g could be obtained with carbon obtained from Jackfruit. While carbon obtained from Coconut fiber and Soap-nut seeds could give the highest capacity of 800 mAh/g and 650 mAh/g, respectively. All other carbon materials gave much lower capacitance. Though the carbon materials obtained from Coconut fiber and Soap-nut seed showed higher values of capacitance in their first cycles, but it was important to know whether these materials can sustain several charging/discharging cycles and whether they could give same amount of the capacitance after several cycles. Therefore, these materials were tried for 100 charging/discharging cycles. Results are shown in Fig. 8. Capacity of Li-ion cell for various charging and discharging process. (A) Represents charging process and (B) represents discharging process. Fig. 8. From Fig. 8, it is observed that except carbon obtained from Soap-nut seeds and Bamboo all others showed rapid decrease in the capacitance just after 5th cycles. The sustainable capacitance after 100th cycles of charging and discharging, obtained with all these carbon materials are shown in Table 1. 3. Results and Discussion: 3.1. Lithium Intercalation Carbon nanomaterials obtained from Soap-nut seeds (Sapindus Mukorossi), Jack Fruit seeds (Artocarpus heterophyllus), Date-seeds (Phoenix acaulis), Neem seeds (Azadirachta indica), Tea leaves (ehretia microphylla), Bamboo stem (Bambusa bambus) and Coconut fiber (Cocos nucifera) were examined for their application in lithium battery. Results of charging/discharging up to 1.5 V and 290 Sunil Bhardwaj et al. / Carbon Letters Vol. 8, No. 4 (2007) 285-291 number of reversible cycle are shown in Fig. 7 and 8. The charging of battery is shown by curve A and that of discharging behavior is shown by curve B. The slops were calculated for charging and discharging curves. It appears that in general, rate of charging is slower than the rate of discharging. The reversibility of the battery was studied by measuring the change in capacity versus the number of cycle under the constant current of 1 mA. At 100th cycles the magnitude of the capacitance available from each of the carbon materials is calculated and the values are shown in the table-1. The examination of these values suggests that carbon materials obtained from the Soap-nut seeds gives the highest capacitance of 130.29 mAh/g. The next highest capacitance i.e. 92.74 mAh/g is obtained with carbon from Bamboo stem The efficiency of charging/discharging process even at 100th cycles was found to be around 96%. This indicates that the cycle stability of Bamboo and Soap-nut seeds in the Li-ion intercalation process is relatively high, as compared to the other carbon material. It is interesting to note that the electrochemical properties of multi walled carbon nano tubes reported from bamboo also showed a good electrochemical properties [19]. In order to understand these behaviors of carbon materials, a graph was plotted between the ratio of intensities of Raman spectra at G- band and D- band (i.e. IG/ID) and the capacitance obtained after 100th cycles (Fig. 9). From the figure 9A it appears that as the magnitude of the IG/ID ratio increases the capacitance of the battery with the carbon materials increases. This suggests that when the carbon materials contain more graphitic carbon, intercalation of lithium is favored resulting into giving higher capacitance. The examination of Raman spectra (Fig. 5) suggests that almost all carbon materials show a large shift in the G-peak from 1575 cm− 1 (as obtained with HOPG) to wards higher side. Therefore another graph was plotted between the difference of peak position of the carbon nanomaterials used from this work and position of the G-peak obtained with HOPG measured under the identical condition (Fig. 9B). This graph shows that as soon as this difference increases more than 20 cm− 1, there is a sharp decrease in the capacitance of the battery, suggesting that the capacitance of the battery (or the efficiency of intercalation and deintercalation of lithium) largely depends upon the graphitic nature of the carbon materials. This also means that the contribution of D-band in the carbon materials should be as low as possible to give higher capacitance. Though XRD of carbon from Bamboo did not show any peak, but it showed a capacitance of 92.74 mAh/g. This suggests that capacity of lithium battery does not entirely depend upon the graphitic nature of carbon. Some other factors like size of pores and/or surface area also plays a role. For this purpose, a graph was plotted between the surface area of the carbon materials and the capacitance of the (A) Graph plotted between the intensities obtained at Gband and D-band (i.e. IG/ID), versus the capacitance obtained after 100th cycles with carbon materials obtained from these precursors (B) Graph showing the relationship between the difference in the G-band peak position of carbon material and G-band peak position obtained with HOPG measured under the identical condition and (C) Graph drawn between the capacitance obtained after the 100th cycles and pore size of the carbon nano materials used for the battery. Fig. 9. battery obtained after 100th cycles. Unfortunately there seems to have no specific trend between the capacitance and the surface area of the carbon nano material (graph not shown here). The reasons could be either there is no such relationship between the surface area and the capacitance or the surface area determined by the methylene blue technique does not give the actual surface area of the material. In absence of facilities to measure the BET surface area, we are not in a position to clarify this point. In our next attempt a graph was plotted between the pore size (as this was obtained from SEM micrographs) and the capacitance after 100th cycles (Fig. 9C). This graph shows a maxima at around 8.1 nm, suggesting that pore size of the material should be around 8 nm. Considering the size of lithium Vander waals radius (0.41 nm), the ratio of pore size (8.1 nm diameter) to the diameter of Van der Waals diameter comes to 9.88. This suggests that pore size (or the cavity) of the carbon nanomaterial should be about 10 times bigger than the diameter of the lithium ion. Smaller or larger than 10 nm would also not be preferred (Fig. 9C). Carbon nanomaterials obtained with Soap-nut seed seems to meet these requirements and hence gives highest capacitance. It can be concluded that the capacity of lithium battery depends upon factors like pore size (i.e., the size of cavity) and graphitic nature of the carbon. Carbon Material from Natural Sources as an Anode in Lithium Secondary Battery 4. Conclusion The analysis of pore size, and capacity of battery suggests that carbon materials should posses certain specific pore size to give an optimum capacitance for a lithium battery. Moreover, carbon materials should possess more graphitic structure and less of D-band to give optimum capacitance. 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