材料科学
电解质
阳极
电镀(地质)
复合材料
无定形固体
微晶
化学工程
集电器
快离子导体
短路
电流密度
金属
冶金
电压
电极
结晶学
化学
工程类
物理化学
地质学
物理
量子力学
地球物理学
作者
Lukas Porz,Tushar Swamy,Brian W. Sheldon,Daniel Rettenwander,Till Frömling,Henry L. Thaman,Stefan Berendts,Reinhard Uecker,W. Craig Carter,Yet‐Ming Chiang
标识
DOI:10.1002/aenm.201701003
摘要
Abstract Li deposition is observed and measured on a solid electrolyte in the vicinity of a metallic current collector. Four types of ion‐conducting, inorganic solid electrolytes are tested: Amorphous 70/30 mol% Li 2 S‐P 2 S 5 , polycrystalline β‐Li 3 PS 4 , and polycrystalline and single‐crystalline Li 6 La 3 ZrTaO 12 garnet. The nature of lithium plating depends on the proximity of the current collector to defects such as surface cracks and on the current density. Lithium plating penetrates/infiltrates at defects, but only above a critical current density. Eventually, infiltration results in a short circuit between the current collector and the Li‐source (anode). These results do not depend on the electrolytes shear modulus and are thus not consistent with the Monroe–Newman model for “dendrites.” The observations suggest that Li‐plating in pre‐existing flaws produces crack‐tip stresses which drive crack propagation, and an electrochemomechanical model of plating‐induced Li infiltration is proposed. Lithium short‐circuits through solid electrolytes occurs through a fundamentally different process than through liquid electrolytes. The onset of Li infiltration depends on solid‐state electrolyte surface morphology, in particular the defect size and density.
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