Deformation and fracture of battery without CFRP layer During TR, the battery shell swells due to the increase of internal pressure P and temperature T. The deformation ε consists of two parts: the deformation ε p produced by internal pressure and the deformation ε t introduced by the thermal expansion effect.
The deformation ε consists of two parts: the deformation ε p produced by internal pressure and the deformation ε t introduced by the thermal expansion effect. The simulation results show that the stress concentration first occurs in the bottom edge of the battery (Fig. 7 a and c).
In the meantime, a finite element model of the battery shell is developed to describe the stress/strain evolution, deformation process, and fracture behavior. The strain rate effect and thermal effect of the battery shell material are considered in the material model.
Deformation and failure of Li-ion batteries can be accurately described by a detailed FE model. The DPC plasticity model well characterizes the granular coatings of the anode and the cathode. Fracture of Li-ion batteries is preceded by strain localization, as indicated by simulation.
The onset of the failure of batteries is understood here as the fracture of the aluminum foil, which triggers the global crack formation. The global geometry of the pouch cell is defined by the radius of the cylindrical indenter and the thickness of the cell . The hardening curve of the aluminum foil is approximated by the power law .
Fracture behaviors of cell shells during thermal runaway are investigated. Experimental characterization validates the physics-based modeling. The shell deformation depends on the inner pressure and temperature distribution. The CFRP sleeve is an effective way to mitigate shell sidewall fractures. 1. Introduction
Battery storage – Shell Climate Change
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DEFORM-3D
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