Acta Phys. -Chim. Sin. ›› 2024, Vol. 40 ›› Issue (3): 2305053.doi: 10.3866/PKU.WHXB202305053
Special Issue: Solid State Batteries
• ARTICLE • Previous Articles Next Articles
Yajie Li1, Bin Chen1, Yiping Wang1, Hui Xing2,3,*(
), Wei Zhao1, Geng Zhang4,*(
), Siqi Shi1,5,6,*(
)
Received:2023-05-29
Revised:2023-07-14
Accepted:2023-07-14
Published:2023-07-31
Contact:
Email: huixing@nwpu.edu.cn (Hui Xing)geng.zhang@kaust.edu.sa (Geng Zhang)sqshi@shu.edu.cn (Siqi Shi)
Supported by:Yajie Li, Bin Chen, Yiping Wang, Hui Xing, Wei Zhao, Geng Zhang, Siqi Shi. Inhibiting Dendrite Growth by Customizing Electrolyte or Separator to Achieve Anisotropic Lithium-Ion Transport: A Phase-Field Study[J]. Acta Phys. -Chim. Sin. 2024, 40(3), 2305053. doi: 10.3866/PKU.WHXB202305053
Table 1
Phase-field simulation parameters."
| Parameter | Symbol | Value | Ref. |
| Interfacial mobility of ξ | Lξ | 2.5 × 10−6 m3∙J−1∙s−1 | |
| Interfacial mobility of φ | Lφ | 5 × 10−8 m3∙J−1∙s−1 | |
| Kinetic coefficient | Lη | 1 s−1 | |
| Barrier height | W | 1.334 × 10−7 J∙m−3 | |
| Gradient energy coefficient 1 | κ0 | 4.17 × 10−5 J∙m−1 | |
| Gradient energy coefficient 2 | κφ | 8.34 × 10−5 J∙m−1 | |
| Anisotropic mode | ω | 4 | |
| Anisotropic strength | r | 0.05 | |
| Charge transfer coefficient | α | 0.5 | |
| Conductivity in electrolyte | σL | 2.67 S∙m−1 | |
| Conductivity in electrode | σS | 1.0 × 10−7 S∙m−1 | |
| Scalar Li+ diffusivity in the electrode | DS | 3.68 × 10−13 m2∙s−1 | |
| Scalar Li+ diffusivity in the electrolyte | DL | 3.68 × 10−10 m2∙s−1 | |
| Faraday constant | F | 9.6485 × 104 C∙mol−1 | |
| Transferred number of electrons | z+ | 1 |
Fig 8
Dendrite growth in electrolytes with inherent anisotropic Li+-diffusion (a–d), and with both inherent and electric potential-induced anisotropic Li+-diffusion (e–h). ${\bar q_{{\rm{de}}}} = 0.34$ in (a, e), ${\bar q_{{\rm{de}}}} = 0.33$ in (b, f), ${\bar q_{{\rm{de}}}} = 0.31$ in (c, g), and ${\bar q_{{\rm{de}}}} = 0.45$ in (d, h)."
Fig 9
Li+ concentration in electrolytes with inherent anisotropic Li+-diffusion (a–d), and with both inherent and electric potential-induced anisotropic Li+-diffusion (e–h). ${\bar q_{\rm{de}}} = 0.34$ in (a, e), ${\bar q_{\rm{de}}} = 0.33$ in (b, f), ${\bar q_{\rm{de}}} = 0.31$ in (c, g), and ${\bar q_{\rm{de}}} = 0.45$ in (d, h)."
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