With current lithium ion batteries optimized for performance under relatively low charge rate conditions, implementation of Extreme Fast Charging (XFC, 6C charging and above) has been hindered by drawbacks including Li plating, kinetic polarization, and heat dissipation. Novel electrode designs, including anodes optimized for rapid lithium diffusion, show promise in alleviating these drawbacks.[1] However, in order to assess potential anode improvements, materials must be characterized in relevant settings, with tools that can discern critical metrics. This submission will detail efforts at Sandia National Lab to assess battery performance under XFC conditions using ultra high precision coulometry to track cycle-to-cycle efficiency and in-cycle dQdV. Efficiency deviations can reveal lithium plating or cathode breakdown, while dQdV measurements can reveal unintended side processes like lithium stripping during discharge. This submission will also describe the need for quick-response temperature control during XFC testing to minimize the effect of cell heating on characterization. Figure 1 shows dQdV vs V on a 5Ah NMC/graphite COTS pouch cell, for charge rates of 0.5C (cycle 3), 1C (cycle 6), and 6C (cycle 24) during a rate capability test. It also shows subsequent 1C discharge cycles, and a 1C/1C cycle after the rate capability (cycle 25). Of note is the particular clarity of the dQdV curves, enabled by high precision coulometry performed on a high precision Arbin battery cycler. Charge curves shift right and peaks become more spread out, which is a consequence of cell polarization at higher charge rates. Discharge curves, however, remain nearly identical throughout cycling, indicating that no lithium stripping processes are seen after increasing charge rates. Figure 2 shows cycling and temperature data for 6C charging / 2C discharge, on the same 5Ah pouch cell type. In this case, rapid response cooling plates are fitted around the cell to reduce cell heating during the high charge rate. The temperature data shows a worst-case temperature rise of only 3oC at the peak of charging along the cell’s edge, which minimizes heating artifacts during cell characterization. [1] S. Ahmed et al, J. Power Sources, 367, 250-262 (2017). Figure 1
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