Starting with the Poisson-Nernst-Planck (PNP) micro-scale equations, a multiple-scale expansion is applied to rigorously derive macroscopic equations of mass and charge transport [3]. Physics-based conditions are identified under which classical macroscale models accurately describe lithium-ion micro-scale dynamics with an accuracy prescribed by the homogenization technique. These conditions are represented schematically in the form of phase diagrams. The temperature-dependent dynamics of lithium-ion battery electrodes are examined using the electrolyte phase diagram [4], and the results obtained indicate that standard macroscopic models fail to describe micro-scale processes in batteries that are operated above critical temperature conditions. The results predicted by analytical studies in previous work [4] are confirmed through numerical simulations in the present work. The equations of the full-homogenized macroscale (FHM) model developed in [3] are resolved using the finite element modeling software COMSOL Multiphysics®. Numerical simulations are performed using the FHM model and the DFN macroscale model developed in COMSOL by Plett [5]. The performance of both models is assessed against data from experiments conducted on 18650 cylindrical lithium-ion cells with nickel manganese cobalt oxide cathode at the Battery Aging and Characterization Laboratory at Clemson University.
2A (1 C-rate) constant current discharge experiments are conducted at 5°C, 23°C, 45°C, and 52°C. The measured battery voltage responses are used to assess the predictive ability of the FHM and DFN models. To prevent any bias, the same geometrical and stoichiometric parameters values are used in both models, and kept constant across different temperatures. For each data set, five parameters are identified for both the models as a function of temperature: electrode diffusion coefficients and reaction rate constants, and contact resistance. The results indicate that the DFN model, which predicts battery dynamics accurately at 5°C and 23°C, fails to replicate the same at 45°C and 52°C towards the end of cell discharge. Simulations results for the performance of both models at these temperatures are illustrated in Fig. 1. The FHM model accurately predicts battery response under all temperature conditions. The lack of accuracy of the DFN model at higher temperatures is due to the inability of the electrolyte equations to capture micro-scale dynamics, indicated by a phase diagram study [4]. The outcome of this work will enable the development of physics-based control strategies to prolong battery useful life for battery management system applications.
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