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Lithium battery internal resistance is a critical parameter reflecting electrochemical performance, influencing power delivery, energy efficiency, and thermal behavior. Accurate measurement of internal resistance helps assess battery health, predict lifespan, and diagnose faults, making it essential in quality control, research, and field maintenance. Various testing methods exist, each with distinct principles, advantages, and applications, tailored to different scenarios from laboratory analysis to in-situ monitoring.
The direct current (DC) discharge method is one of the most straightforward techniques. It involves applying a known DC current to the battery and measuring the voltage drop before and during discharge. Internal resistance (R) is calculated using Ohm’s law: R = ΔV / I, where ΔV is the voltage difference and I is the discharge current. For example, a 3.7V lithium cell discharged at 1A with a voltage drop from 3.7V to 3.5V yields an internal resistance of 0.2Ω. This method is simple to implement with basic equipment (power supplies, multimeters) and is widely used in production lines for rapid screening. However, it has limitations: it measures only the DC resistance, which includes ohmic resistance but not the frequency-dependent polarization resistance, and it can cause temporary capacity loss due to discharge.
The alternating current (AC) impedance spectroscopy method, also known as electrochemical impedance spectroscopy (EIS), provides a more comprehensive analysis by measuring resistance across a range of frequencies (typically 10mHz to 1MHz). A small AC signal is applied to the battery, and the resulting voltage response is analyzed to generate an impedance spectrum (Nyquist plot). This plot distinguishes between ohmic resistance (Rₛ), charge transfer resistance (Rct), and diffusion resistance (Warburg impedance), offering insights into internal electrochemical processes. For instance, an increase in Rct may indicate electrode degradation, while a larger Warburg impedance suggests slowed ion diffusion. EIS is highly accurate and non-destructive, making it ideal for research and detailed health assessments. However, it requires specialized equipment (potentiostats/galvanostats) and complex data interpretation, limiting its use in real-time monitoring.
The load pulse method combines elements of DC and AC testing, using short current pulses to measure resistance. A high-current pulse (e.g., 10C for 1–5 seconds) is applied, and the voltage transient is recorded. The internal resistance is calculated from the voltage drop during the pulse (ohmic resistance) and the subsequent recovery (polarization resistance). This method simulates real-world conditions, such as EV acceleration, making it relevant for performance evaluation. It balances accuracy and practicality, used in BMS systems for in-situ resistance monitoring. For example, EV BMS often employs 1-second 5C pulses to estimate resistance, adjusting power output based on the results. The main challenge is minimizing pulse duration to avoid significant capacity loss while ensuring measurable voltage changes.
The four-wire (Kelvin) measurement technique enhances accuracy by eliminating contact resistance. It uses two wires to carry current and two separate wires to measure voltage, isolating the voltage sensing from the current path. This is particularly useful for low-resistance measurements (below 1mΩ) in large battery packs, where contact resistance between test probes and terminals can skew results. Automated battery testers often integrate four-wire sensing to ensure precision in production and quality control.
lithium battery internal resistance testing methods vary in complexity and application: DC discharge for simplicity, EIS for detailed electrochemical analysis, load pulse for real-world simulation, and four-wire measurement for high precision. Selecting the appropriate method depends on the testing goals, equipment availability, and whether the battery is in production, research, or operational use.
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