过充锂离子电池阻抗诊断

C. Love, K. Swider-Lyons
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引用次数: 41

摘要

我们使用电化学阻抗谱(EIS)来监测锂离子电池在过充电期间和过充电后的电阻增加。EIS通常用于测量锂离子电池内部的电阻,并可以显示由大块电极、电解质以及电极/电解质界面内发生的化学和电化学反应引起的电阻行为变化[1]。电化学电池中的物理过程具有不同的时间常数或有效电容,从而导致不同的频率响应[2]。我们报告了过充电池的阻抗特性与健康电池的阻抗特性明显不同。在500hz时,结果与健康电池的充电状态无关,与过度充电的电池截然不同[3]。500hz的变化不是巧合,因为这个频率响应过充电时形成的电池钝化层。根据测试结果,我们建议使用基于单点阻抗的诊断工具来监测电池的健康状况。商业锂离子柱状电池(Full River 10至300毫安时)用于这些实验。EIS测量数据采集使用由EG&G PAR263A恒电位器驱动的Solartron SI 1260阻抗增益相位分析仪。在开路条件下,在充电、过充和放电的不同电压下,在50 kHz和10 mHz之间采用±10 mV的振幅扰动收集阻抗数据。充电电压上限为4.2 V ~ 5.0 V,放电电压截止在2.8 V恒定。EIS数据由ZPlot和ZView软件包(Scribner Associates Inc.)收集和分析。电池在大约23°C下以恒定1C速率(30 mA)充电和放电。使用Maccor系列4300电池测试仪测量重复充电/放电(2.8 - 4.2 V)和过充电/放电(2.8 - 4.4、4.6、4.8、5.0 V)数据。与正常工作的LiCoO2|C电池(充电在2.8 - 4.2 V之间)相比,过度充电的LiCoO2|C电池具有截然不同的阻抗谱。与推荐的4.2 V充电上限相比,软过充电至4.4 V会导致阻抗谱的微小变化。当过充电高于4.4 V时,阻抗特性发生显著变化。阻抗谱的形状不可逆转地改变后在排放严重的5.0 V超载,不再像电池的阻抗谱测量4.2 V(见参考3)。这种不可逆性在充电锂离子电池的阻抗响应是在500 Hz最为明显(图1)。一个过度充电4.6 V导致电池阻抗在500 Hz显著下降,这反映出电极钝化层的结构的变化。随着进一步的过充循环,500hz的电池阻抗增加,反映了电池电阻的增加,这是过热电池的第一步。这些趋势与10到300毫安时的电池尺寸无关,但需要做更多的工作来确定不同化学物质(即LiFePO4阴极)、电池组和不同温度下的电池的这些趋势。这项工作为锂离子电池的安全运行提供了一个简单的预测和诊断,也为电池过度充电失败的原因提供了一些信息。
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Impedance Diagnostic for Overcharged Lithium-Ion Batteries
We use electrochemical impedance spectroscopy (EIS) to monitor the resistance increases associated with Li-ion batteries during and after overcharge. EIS is commonly used to measure the resistance within a Li-ion cell and can show changes in resistance behavior originating from chemical and electrochemical reactions occurring within bulk electrodes, electrolyte, and along electrode/electrolyte interfaces [1]. The physical processes in electrochemical cells have different time constants or effective capacitances, which result in different frequency responses [2]. We report the impedance characteristics for overcharged batteries are markedly different from those of the healthy batteries. At 500 Hz, the results are independent of state of charge for healthy batteries, and grossly different for overcharged batteries [3]. The changes at 500 Hz are not coincidental, as this frequency responsive to the cell passivation layers that form upon overcharge. From the results, we recommend a singlepoint impedance-based diagnostic tool for monitoring battery health. Commercial Li-ion prismatic cells (Full River 10 to 300 mAh) are used for these experiments. EIS measurements were collected using a Solartron SI 1260 impedance gain-phase analyzer driven by an EG&G PAR263A potentiostat. Impedance data were collected under open circuit conditions using a ±10 mV amplitude perturbation between 50 kHz and 10 mHz at various voltages during charge, overcharge and discharge. The upper limit for the charge voltage ranged from 4.2 V to 5.0 V, while the discharge voltage cutoff was held constant at 2.8 V throughout all experiments. EIS data were collected and analyzed by ZPlot and ZView software packages (Scribner Associates Inc.). The batteries were charged and discharged at constant 1C rates (30 mA) at approximately 23°C. Repeated charge/discharge (2.8–4.2 V) and overcharge/discharge (2.8 – 4.4, 4.6, 4.8, 5.0 V) data were measured using a Maccor Series 4300 battery tester. Overcharged LiCoO2|C cells have drastically different impedance spectra as compared to properly operated ones (charged between 2.8 – 4.2 V). A soft overcharge to 4.4 V results in small changes in the impedance spectrum compared to the recommended 4.2 V upper charging limit. When overcharged above 4.4 V, the impedance characteristics change dramatically. The shapes of the impedance spectra irreversibly change upon discharge after a severe 5.0 V overcharge and no longer resemble the impedance spectra measured for the battery charged to 4.2 V (see reference 3). This irreversibility in the impedance response for overcharged Li-ion cells is most pronounced at 500 Hz (Fig 1). A single overcharge to 4.6 V causes the battery impedance at 500 Hz to drop significantly, reflecting a change in the structure of the electrode passivation layers. With further overcharge cycles, the battery impedance at 500 Hz increases, reflecting an increase in the cell resistance, and the first steps toward an overheating battery. These trends are independent of battery sizes from 10 to 300 mAh, but more work is needed to determine these trends across different chemistries (i.e. LiFePO4 cathodes), battery packs, and for cells operating at different temperatures. This work points to a simple prognostic and diagnostic for the safe operation of Li-ion batteries, and also sheds some information on the causes of overcharge failure in batteries.
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Electrochemical and Solid State Letters
Electrochemical and Solid State Letters 工程技术-材料科学:综合
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