Author
Listed:
- Ziyang Ning
(University of Oxford
Fujian Science & Technology Innovation Laboratory for Energy Devices (21C Lab))
- Guanchen Li
(University of Oxford
University of Glasgow
The Faraday Institution, Harwell Campus)
- Dominic L. R. Melvin
(University of Oxford
The Faraday Institution, Harwell Campus)
- Yang Chen
(University of Oxford
University of Bath)
- Junfu Bu
(University of Oxford
The Faraday Institution, Harwell Campus)
- Dominic Spencer-Jolly
(University of Oxford
The Faraday Institution, Harwell Campus)
- Junliang Liu
(University of Oxford)
- Bingkun Hu
(University of Oxford)
- Xiangwen Gao
(University of Oxford
The Faraday Institution, Harwell Campus)
- Johann Perera
(University of Oxford)
- Chen Gong
(University of Oxford)
- Shengda D. Pu
(University of Oxford)
- Shengming Zhang
(University of Oxford)
- Boyang Liu
(University of Oxford
The Faraday Institution, Harwell Campus)
- Gareth O. Hartley
(University of Oxford
The Faraday Institution, Harwell Campus)
- Andrew J. Bodey
(Diamond Light Source, Harwell Campus)
- Richard I. Todd
(University of Oxford)
- Patrick S. Grant
(University of Oxford
The Faraday Institution, Harwell Campus)
- David E. J. Armstrong
(University of Oxford
The Faraday Institution, Harwell Campus)
- T. James Marrow
(University of Oxford)
- Charles W. Monroe
(University of Oxford
The Faraday Institution, Harwell Campus)
- Peter G. Bruce
(University of Oxford
The Faraday Institution, Harwell Campus
University of Oxford)
Abstract
All-solid-state batteries with a Li anode and ceramic electrolyte have the potential to deliver a step change in performance compared with today’s Li-ion batteries1,2. However, Li dendrites (filaments) form on charging at practical rates and penetrate the ceramic electrolyte, leading to short circuit and cell failure3,4. Previous models of dendrite penetration have generally focused on a single process for dendrite initiation and propagation, with Li driving the crack at its tip5–9. Here we show that initiation and propagation are separate processes. Initiation arises from Li deposition into subsurface pores, by means of microcracks that connect the pores to the surface. Once filled, further charging builds pressure in the pores owing to the slow extrusion of Li (viscoplastic flow) back to the surface, leading to cracking. By contrast, dendrite propagation occurs by wedge opening, with Li driving the dry crack from the rear, not the tip. Whereas initiation is determined by the local (microscopic) fracture strength at the grain boundaries, the pore size, pore population density and current density, propagation depends on the (macroscopic) fracture toughness of the ceramic, the length of the Li dendrite (filament) that partially occupies the dry crack, current density, stack pressure and the charge capacity accessed during each cycle. Lower stack pressures suppress propagation, markedly extending the number of cycles before short circuit in cells in which dendrites have initiated.
Suggested Citation
Ziyang Ning & Guanchen Li & Dominic L. R. Melvin & Yang Chen & Junfu Bu & Dominic Spencer-Jolly & Junliang Liu & Bingkun Hu & Xiangwen Gao & Johann Perera & Chen Gong & Shengda D. Pu & Shengming Zhang, 2023.
"Dendrite initiation and propagation in lithium metal solid-state batteries,"
Nature, Nature, vol. 618(7964), pages 287-293, June.
Handle:
RePEc:nat:nature:v:618:y:2023:i:7964:d:10.1038_s41586-023-05970-4
DOI: 10.1038/s41586-023-05970-4
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Cited by:
- Daems, K. & Yadav, P. & Dermenci, K.B. & Van Mierlo, J. & Berecibar, M., 2024.
"Advances in inorganic, polymer and composite electrolytes: Mechanisms of Lithium-ion transport and pathways to enhanced performance,"
Renewable and Sustainable Energy Reviews, Elsevier, vol. 191(C).
- Han Su & Jingru Li & Yu Zhong & Yu Liu & Xuhong Gao & Juner Kuang & Minkang Wang & Chunxi Lin & Xiuli Wang & Jiangping Tu, 2024.
"A scalable Li-Al-Cl stratified structure for stable all-solid-state lithium metal batteries,"
Nature Communications, Nature, vol. 15(1), pages 1-10, December.
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