Journal of New Materials for Electrochemical Systems 6, 259-262 (2003) © J. New. Mat. Electrochem. Systems A New Synthetic Method for Preparing LiFePO with Enhanced Electrochemical Performance 4 Z.P. Guoa, H. Liub, S. Bewlaya, H.K. Liua, and S.X. Doua aInstitute for Superconducting & Electronic Materials, University of Wollongong, NSW 2522, Australia of Materials Science and Engineering, Sichuan University, Chengdu 610065, China bCollege (Received June 2, 2003; received revised form November 6, 2003) Abstract: The paper describes the synthesis and the properties of LiFePO4 cathode material prepared by a novel modified solid-state reaction. The novel aspect of the synthesis is based on the addition of a growth inhibitor (citric acid) to the precursor. The citric acid addition does not affect the structure of the cathode but considerably improves its electrochemical performances because small particle size powders are obtained. A cell discharged at 17 mA/g was able to deliver a specific capacity of 167 mAh/g with good capacity retention. EIS experiments verified that the charge transfer has been improved compared to the sample prepared by the conventional solid-state reaction. Key words: LiFePO4, Citric acid, growth inhibitor In this study, we describe a novel modified solid-state reaction to prepare nanosized LiFePO4 with enhanced electrochemical performance in terms of the specific capacity and charge/ discharge rate. The basic idea is that citric acid added to the precursors could limit the growth of the LiFePO4 particles and thus help in obtaining samples with low and uniform particle sizes. The modified solid-state reaction has been described previously by this group as a method for preparing other electroactive materials such as LiCoO2, LiMnO2, etc. [5, 6]. We believe the modified solid-state method provides an extremely promising general method for the mass production of lithiated transition metal compounds. 1. INTRODUCTION Since the pioneering study of Padhi et al. [1], lithium transition metal phosphates have become of great interest as storage cathodes for rechargeable lithium batteries. Among these materials, LiFePO4 is one of the most promising compounds due to its high density, the low cost of the starting materials, the relative absence of toxicity, and the fact that the intermediate voltage value (3.45V vs Li) at which it operates makes it stable in most of the organic electrolytes usually employed. However, this cathode was strictly related to the current density used, associated with diffusion -controlled kinetics of the electrochemical process. Based on previous studies, a reduction in the grain size could be one possible route to improve the performance of LiFePO4, as the slow lithium ion diffusion in LiFePO4 is the main cause of the poor electrochemical performance [2-4]. 2. EXPERIMENTAL 2.1. Powder preparation The LiFePO4 compounds were prepared using a modified solid-state reaction. Stoichiometric Fe(COO)2.2H2O, (NH4)2HPO4, Li2CO3, and citric acid with Li:citric acid =1:1 were ball milled for 12 h in a planetary mill with agate vessels. The resulting product was first decomposed at 350 °C *To whom correspondence should be addressed: E-mail: [email protected]; Fax: 61 2 4221 5731 259 260 Z.P. Guo et al. / J. New. Mat. Electrochem. Systems 6, 259-262 (2003) for 10h to expel the gases, then the mixture was ground and pressed into pellets. The pellets were then fired in a purified Ar flow at various temperatures from 650°C to 800°C for 24 h. 011 020 Phase analysis was carried out by powder X-ray diffraction (XRD) with Cu Kα radiation in a Philips 1730 X-ray diffractometer. Scanning electron micrographs (SEM) were obtained to examine the morphology of the powder. The Brunauer, Emmett, and Teller (BET) method was used to measure the surface area of powders. 120 111 121 021 200 041 211 031 101 800oC 131 221 140 012 112 022 700oC 600oC 15 20 25 30 35 40 45 2 - T het a / d eg r ee 2.2. Electrochemical measurements 3. RESULTS AND DISCUSSION 3.1. Crystal structure The main limitation with respect to this compound is its very poor electronic conductivity which limits the cycling capability. Several methods have been proposed to solve this problem, such as carbon coating or thin metal particle dispersion. But the amount of carbon recover the theoretical capacity (~20 %) and the metal used (copper or silver) are much more expensive than the cathode material itself [7,8]. LiFePO4 compounds synthesized by the modified solid-state reaction could overcome the disadvantages above, as well as provide impressive electrochemical performance. Figure 1a. X-ray diffraction patterns of LiFePO4 prepared by modified solid state reaction and sintered at 600°C, 700°C and 800°C. Intensity / Arb. unit A cathode was prepared by mixing LiFePO4 powder with 20 wt% carbon black and 5 wt% PVDF (polyvinylidene fluoride) solution. The LiFePO4 and carbon black powders were first added to a solution of PVDF in N-methyl-2pyrrolidinone (NMP) to make a slurry with appropriate viscosity. Al foil was then used to coat the mixture. After the electrode was dried at 140 °C for 2 h in vacuum, it was compressed at a rate of about 150 kg/cm2. Teflon test cells were assembled in an argon filled glove box, where the counter electrode was Li metal and the electrolyte was 1M LiPF6 dissolved in a 50/50 vol% mixture of ethylene carbonate (EC) and dimethyl carbonate (DMC). These cells were cycled between 2.0 and 4.4 V at room temperature to measure the electrochemical response. In order to measure the electrochemical impedance response, an EG&G Model 6310 electrochemical impedance analyzer was used, and electrochemical impedance software (Model 398) was used to control a computer for conductivity and stability measurements. After the electrode attained an steady-state potential, electrochemical impedance measurements were carried out by applying an ac voltage of 5 mV over a frequency range from 1 mHz to 100 kHz. 350oC 10 20 30 40 50 60 70 2-Theta / degree Figure 1b. X-ray diffraction pattern of LiFePO4 prepared by modified solid state reaction and sintered at 350°C. Although a single phase of olivine was obtained (from the xray patterns) at various temperatures, the cathode performance depended strongly on the sintering temperatures. Samples synthesized above 800 °C show good performance as shown in Figure 2. The reversible capacity of 164 mAh/g (167 mAh/ g for initial discharge) for compounds sintered at 800 °C is almost equal to the theoretical capacity of LiFePO4 (170 mAh/ g), while samples sintered at 600 °C and 700 °C had capacities of 97 and 149 mAh/g, respectively. To explain this phenomenon from the structural aspect, the diffraction patterns were refined based on an ordered olivine structure 200 18 0 16 0 14 0 12 0 Figure 1 shows the x-ray diffraction data collected for LiFePO4 materials. X-ray analysis shows that the sample heat treated at 350 °C is completely amorphous. Further heated the samples from 600 °C to 800 °C, the x-ray diffraction patterns show a series of diffraction peaks, which indicate that a transformation from an amorphous to a crystalline phase occurred. Single phase LiFePO4 compounds were obtained at temperatures from 600 to 800 °C. 10 0 80 60 40 20 0 500 550 600 650 700 750 Sint er ing T emp er at ur e/ 800 o 850 900 950 C Figure 2. Change in capacity (1st discharge) as a function of sintering temperature. 261 A New Synthetic Method for Preparing LiFePO / J. New. Mat. Electrochem. Systems 6, 259-262 (2003) 4 comprising PO4 tetrahedra and distorted FeO6 octahedra, which produce a two-dimensional pathway for lithium-ion diffusion. The refined relative cell parameters for the LiFePO4 samples are plotted versus the synthesis temperature (Fig. 3). The relative lattice parameters are normalized to the respective values of the sample synthesized at 600 °C, in order to illustrate the temperature dependency more clearly. The absolute lattice parameters for this reference material are a = 10.298 Å, b = 5.993 Å, c = 4.685 Å. The lattice parameters a and c decrease slightly with increased synthesis temperature, whereas the lattice parameter b is unaffected. This result may indicate the existence of an unidentified stoichiometric or structural deviation from the ideal olivine type LiFePO4, which depends on the synthesis temperature. On the other hand, based on Yamada’s theory [9], samples sintered below 800 °C could contain Fe3+ impurity phase, which appeared amorphous or nano-particulate because it was not detectable by x-ray diffraction. The existence of trivalent Fe, which might be formed by a small amount of oxygen included in the argon flow and/or residual air trapped in the small pores of the particles, decreases the charge-discharge capacity, as shown in Figure 2. 1.0001 1.0000 Relative lattice dimension 0.9999 0.9998 0.9997 0.9996 0.9995 0.9994 o a/a(600 C) o b/b(600 C) o c/c(600 C) 0.9993 0.9992 0.9991 0.9990 600 650 700 750 800 Synthesis temperature Figure 3. Influence of the synthesis temperature on relative lattice parameters of different samples, sintered at different temperatures. For clarity, the lattice constants are normalized to the respective values for the material synthesized at 600°C. The absolute values for this reference material are a=10.298Å, b=5.993Å, c=4.685Å. It was also reported that LiFePO4 particles would have an abrupt increase in size when the sintering temperature is above 600 °C, which could result in a sharp decrease in material capacity [9]. However, we did not observe this phenomenon because the citric acid added to the precursors works as a growth inhibitor, which significantly reduced the particle size. There is no obvious increase in particle growth even at 900 °C. Figure 4. SEM micrograph of LiFePO4 obtained by modified solid-state reaction. 3.2. Electrochemical characteristics Figure 5 shows the voltage profiles of a LiFePO4 sample as a function of the specific capacity for several discharge rates. The cell was discharged galvanostatically under different specific currents, ranging from C/10 to 3C. The discharge and charge cut-off voltages are 2.0 and 4.5 V, respectively. The cell was always recharged at the same specific current of 17 mA/g to assure identical initial conditions for any discharge. At the lowest specific discharge current used (17 mA/g), the cell was able to deliver a specific capacity of 167 mAh/g based on the active material weight only. By increasing the current density the utilization of the active material decreased, and about 145 mAh/g was delivered at a specific current of 3C. This result is very good when compared with iron phosphate synthesized by traditional solid state chemistry, in which an increase in the discharge current results in severe capacity fading. This effect was claimed to have a kinetic origin because the full capacity was recovered on returning to a lower current density. The excellent performance of the samples is due to the small particle sizes achieved by the modified solid-state synthesis. Small particles lead to a large surface area of LiFePO4 (29 m2/ g), which makes better contact between the particles and electrolyte, and it helps to accelerate the lithium diffusion in 5 4.5 4 3.5 3 2.5 2 3C C/ 10 1 0.5 0 0 Figure 4 is a typical SEM micrographs for samples sintered at 800 °C. The materials are characterized by a globular structure with a grain size of about 100 nm. BET analysis gives a specific surface area of 29 m2/g. 1C 1.5 20 40 60 80 100 120 140 160 180 Sp ecif ic cap acit y / A h/ Kg Figure 5. Rate capability test of LiFePO4 compounds, synthesized by modified solid state reaction. 262 Z.P. Guo et al. / J. New. Mat. Electrochem. Systems 6, 259-262 (2003) the LiFePO4 structure [10]. Long–term cycling of the LiFePO4 compounds confirmed the excellent reversibility of the insertion reaction. As shown in Figure 6, the cycle retention rate of LiFePO4 is 92 % after 50 charge-discharge cycles. 180 160 140 120 100 80 60 40 20 0 1 3 5 7 9 11 13 15 17 19 21 23 25 27 29 31 33 35 37 39 41 43 45 47 49 4. CONCLUSION The results reported demonstrate that the electrode response of the phosphor-olivine LiFePO4 cathode may be enhanced by a novel modified solid-state reaction synthesis procedure. Citric acid addition does not affect the structure of the cathode but it appears to favor the growth of small particles. This in turn improves the electrochemical performance of the LiFePO4 electrode. A cell discharged at 17 mA/g was able to deliver a specific capacity of 167 mAh/g with good capacity retention. EIS experiments verified that the charge transfer has been improved compared to the sample prepared by conventional solid-state reaction. Work is in progress in our laboratory to understand the mechanism of lithium insertion into this very promising cathodic material for lithium ion batteries. C ycle numb er Figure 6. Cycling test of LiFePO4 synthesized by the modified solid state reaction (sintered at 800 °C, charged-discharged at a C/10 rate). To investigate the kinetics of the electrode process, AC impedance measurements were conducted. EIS experiments were performed on working electrodes in the OCV state. Compared to the LiFePO4 sample prepared by conventional solid state reaction, the EIS experiments performed on LiFePO4 samples prepared by modified solid state reaction (Fig. 7) show clearly that the charge transfer has been improved. The charge transfer resistance varies from 500 Ω (conventional sample) to 200 Ω (sample prepared by modified solid state reaction). More measurements are needed to understand the mechanism of lithium insertion into this very promising cathodic material for lithium ion batteries. Recent work performed in our laboratory involving synthesis of substituted-LiFeO4 (such as Mg) using the modified solid-state reaction is very promising in terms of enhancement of the conductivity of the material. This should allow very good electrochemical performance. The details will be published elsewhere. -1000 -800 Zim / ohm -600 -400 -200 0 0 200 400 600 800 1000 ZR / ohm Figure 7. EIS spectra of LiFePO4 cathodes, o: prepared by conventional solid state reaction; ∆: prepared by modified solid state reaction. REFERENCES [1] A. K. Padhi, K. S. Nanjundaswamy and J. B. Goodenough, J. Electrochem. Soc. 144, 1188 (1997). [2] A. S. Andersson, L. Haggstrom, B. Kalska, J. O. Thomas, Electrochem. Solid-State Lett. 3, 66 (2000). [3] P. Prosini, D. Zane, M. Pasquali, Electrochim. Acta 46, 3517 (2001). [4] S. Yang, Y. Song, D.Y. Zavalij, M.S. Whittingham, Electrochem. Comm. 4, 239 (2002). [5] Z. P. Guo, G.X. Wang, K. Konstantinov, H.K. Liu, S.X. Dou, J. Alloy and Compounds 346, 255 (2002). [6] X. Xia, Z. P. Guo, N. Yanna, J. New Mat. Electrochem. Systems 3, 327 (2000). [7] H. Huang, S.-C. Yin, L. F. Nazar, Electrochem. Solid-State Lett. 4(10), A170 (2001). [8] F. Croce, A. D’. Epifanio, J. Hassoun, A. Deptula, T. Olczac, B. Scrosati, Electrochem. Solid-State Lett. 5 (3), A47 (2002). [9] A. Yamada, S. C. Chung, K. Hinokuma, J. Electrochem. Soc. 148(3), A224 (2001). [10] Y. S. Lee and M. Yoshio, Electrochem Solid-State Lett. 4(10), A166 (2001).
© Copyright 2026 Paperzz