液体浸没冷却条件下锂离子电池片的热性能

N.P. Williams, D. Trimble, S.M. O’Shaughnessy
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引用次数: 0

摘要

实验研究了26650 LiFePO4圆柱形锂离子电池在直接接触液浸冷却条件下的充电和放电过程中电极端子或电极片的热性能,突出了它们对电池整体传热的贡献,这是以前没有研究过的。由于电池的各向异性热物理特性,再加上来自电气连接的额外加热,在Novec 7000中完全浸入时,终端表面的传热率很高。初始体积流体温度为33°C ± 0.5°C的两相条件的建立进一步增强了传热,在终端表面诱导核沸腾时,在整个电池中提供了更大的热均匀性。剧烈的蒸汽泡生长和离开限制了终端与散装流体之间的温差,表明传热强度,其值比自然对流液体浸泡条件下观察到的值低2到3倍。当放电速率为10C时,相变使正负极与体流体的温差最大分别限制在3.5℃和5℃以内。相应的电池热不均匀性保持在2.2°C,最大限度地减少了加速的电化学材料降解。在以4C的速率充电时也表现出类似的性能,将正极和负极与散装流体之间的温差分别限制在1.4°C和2.2°C以内,并将电池热不均匀性限制在1°C以内。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Thermal performance of lithium-ion battery tabs under liquid immersion cooling conditions
The thermal performance of the electrode terminals or tabs of a 26650 LiFePO4 cylindrical lithium-ion battery under direct contact liquid immersion cooling conditions is experimentally investigated during charging and discharging, highlighting their contribution to the overall heat transfer from the battery which has not been examined previously. High rates of heat transfer occur from the terminal surfaces for complete immersion in Novec 7000 due to the battery’s anisotropic thermophysical properties, coupled with additional heating from the electrical connections. The establishment of two-phase conditions for initial bulk fluid temperatures of 33 °C ± 0.5 °C further augments the heat transfer, providing greater thermal uniformity across the entire battery as nucleate boiling is induced on the terminal surfaces. Vigorous vapour bubble growth and departure limits the temperature difference between the terminals and the bulk fluid, indicative of the heat transfer intensity, with values two to three times lower than those observed under natural convection liquid immersion conditions. For the discharge rate of 10C, the phase change restricts the temperature difference between the positive and negative terminals and the bulk fluid to a maximum of 3.5 °C and 5 °C respectively. A corresponding cell thermal inhomogeneity of 2.2 °C is maintained, minimising accelerated electrochemical material degradation. Similar performance is exhibited during charging at the rate of 4C, restricting the temperature difference between the positive and negative terminals and the bulk fluid to a maximum of 1.4 °C and 2.2 °C respectively, and the cell thermal inhomogeneity to 1 °C.
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