Thermal Properties of Lithium‐Ion Battery and Components

Experimental thermal property data of the Sony US-18650 lithium-ion battery and components are presented, as well as thermal property measuring techniques. The properties in question are specific heat capacity (C{sub p}), thermal diffusivity ({alpha}), and thermal conductivity ({kappa}), in the presence and absence of electrolyte [1 M LiPF{sub 6} in ethylene carbonate-dimethyl carbonate (EC:DMC, 1:1 wt %)]. The heat capacity of the battery, C{sub p}, is 0.96 {+-} 0.02 J/g K at an open-circuit voltage (OCV) of 2.75 V, and 1.04 {+-} 0.02 J/g K at 3.75 V. The thermal conductivity, {kappa}, was calculated from {kappa} {identical_to} {alpha}{rho}C{sub p} where {alpha} was measured by a xenon-flash technique. In the absence of electrolyte, {kappa} increases with OCV, for both the negative electrode (NE) and the positive electrode (PE). For the NE, the increase is 26% as the OCV increases from 2.75 to 3.75 V, whereas for the PE the increase is only 5 to 6%. The dependence of both C{sub p} and {kappa} on OCV is explained qualitatively by considering the effect of lithiation and delithiation on the electron carrier density, which leads to n-type semiconduction in the graphitic NE material, but a change from semiconducting to metallic character in Li{submore » x}CoO{sub 2} PE material. The overall effect is an increase of C{sub p} and {kappa} with OCV. For {kappa} this dependence is eliminated by electrolyte addition, which, however, greatly increases the effective {kappa} of the layered battery components by lowering the thermal contact resistance. For both NE and PE, the in-plane {kappa} value (measured along layers) is nearly one order of magnitude higher than the cross-plane {kappa}. This is ascribed mostly to the high thermal conductivity of the current collectors and to a lesser extent to the orientation of particles in the layers of electrodes.« less