中国机械工程 ›› 2026, Vol. 37 ›› Issue (3): 708-716.DOI: 10.3969/j.issn.1004-132X.2026.03.020
收稿日期:2025-02-22
出版日期:2026-03-25
发布日期:2026-04-08
通讯作者:
王东城
作者简介:王国栋,男,1994年生,博士研究生。研究方向为锂离子电池极片辊压工艺。E-mail: wangguodong0150@163.com基金资助:
WANG Guodong1(
), WANG Dongcheng1,2(
), DUAN Bowei1, LIU Hongmin1
Received:2025-02-22
Online:2026-03-25
Published:2026-04-08
Contact:
WANG Dongcheng
摘要:
辊压是锂离子电池极片制造过程中的重要工序,辊压力是极片辊压的重要参数,由于电池极片的特殊结构,辊压力难以预测。为解决这一问题,基于粉末成形领域的Kuhn屈服准则,建立了一种锂离子电池极片辊压过程单位压力分布预测模型,并通过辊压实验对模型进行了验证。结果表明,模型计算结果与实验数据吻合良好,对单位宽度压力的预测误差保持在10%以内。进一步研究分析了辊缝内单位压力与摩擦应力分布特征,分别讨论了压下率与轧辊直径对单位宽度压力与单位宽度力矩的影响,研究结果显示,随着压下率和轧辊直径的增大,单位宽度压力与单位宽度力矩均随之增大。
中图分类号:
王国栋, 王东城, 段伯伟, 刘宏民. 基于Kuhn屈服准则的锂离子电池极片辊压力建模与分析[J]. 中国机械工程, 2026, 37(3): 708-716.
WANG Guodong, WANG Dongcheng, DUAN Bowei, LIU Hongmin. Modeling and Analyses of Calendering Pressure for Lithium-ion Battery Electrodes Based on Kuhn Yield Criterion[J]. China Mechanical Engineering, 2026, 37(3): 708-716.
| 低压站 | 高压站 | |
|---|---|---|
| 压力变化范围/Pa | 0~3.45×105 | 大气压~2.28×108 |
| 分辨率/Pa | 68.9 | 689 |
| 孔径测量范围/μm | 3.6~360 | 0.005~6 |
表1 压汞仪参数
Tab.1 Mercury intrusion porosimeter parameters
| 低压站 | 高压站 | |
|---|---|---|
| 压力变化范围/Pa | 0~3.45×105 | 大气压~2.28×108 |
| 分辨率/Pa | 68.9 | 689 |
| 孔径测量范围/μm | 3.6~360 | 0.005~6 |
| σ0/MPa | n | K/MPa | s | m | ρ0 | |
|---|---|---|---|---|---|---|
| 正极 | 410 | 3.5 | 4200 | 1 | 4 | 0.581 |
| 负极 | 153 | 2.5 | 700 | 1 | 6 | 0.461 |
表2 涂层参数
Tab.2 Coating parameters
| σ0/MPa | n | K/MPa | s | m | ρ0 | |
|---|---|---|---|---|---|---|
| 正极 | 410 | 3.5 | 4200 | 1 | 4 | 0.581 |
| 负极 | 153 | 2.5 | 700 | 1 | 6 | 0.461 |
| 轧辊直径/mm | 极片类型 | A | B |
|---|---|---|---|
| 110 | 正极 | 0.357 | 352.77 |
| 负极 | 0.571 | 127.99 | |
| 130 | 正极 | 0.329 | 314.41 |
| 负极 | 0.605 | 152.28 |
表3 Kawakita方程拟合参数
Tab.3 Fitting parameters of the Kawakita equation
| 轧辊直径/mm | 极片类型 | A | B |
|---|---|---|---|
| 110 | 正极 | 0.357 | 352.77 |
| 负极 | 0.571 | 127.99 | |
| 130 | 正极 | 0.329 | 314.41 |
| 负极 | 0.605 | 152.28 |
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