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静电场驱动下液体薄膜的几何形状

E·M·田 T·P·斯沃博德内 J·D·菲利普斯

E·M·田, T·P·斯沃博德内, J·D·菲利普斯. 静电场驱动下液体薄膜的几何形状[J]. 应用数学和力学, 2011, 32(8): 973-980. doi: 10.3879/j.issn.1000-0887.2011.08.008
引用本文: E·M·田, T·P·斯沃博德内, J·D·菲利普斯. 静电场驱动下液体薄膜的几何形状[J]. 应用数学和力学, 2011, 32(8): 973-980. doi: 10.3879/j.issn.1000-0887.2011.08.008
Emily M. Tian, Thomas P. Svobodny, Jason D. Phillips. Thin Liquid Film Morphology Driven by Electro-Static Field[J]. Applied Mathematics and Mechanics, 2011, 32(8): 973-980. doi: 10.3879/j.issn.1000-0887.2011.08.008
Citation: Emily M. Tian, Thomas P. Svobodny, Jason D. Phillips. Thin Liquid Film Morphology Driven by Electro-Static Field[J]. Applied Mathematics and Mechanics, 2011, 32(8): 973-980. doi: 10.3879/j.issn.1000-0887.2011.08.008

静电场驱动下液体薄膜的几何形状

doi: 10.3879/j.issn.1000-0887.2011.08.008
详细信息
  • 中图分类号: O357.1

Thin Liquid Film Morphology Driven by Electro-Static Field

  • 摘要: 利用六边形-俯视图的弱非线性稳定性分析和数值仿真,在电场作用下,研究高分子薄膜表面静态模式的发展过程.在无限空间域上,空间和高分子薄膜之间的界面,由薄膜方程给出其随时间的演变,综合考虑了电力的驱动和表面张力的传播.非线性界面的增长包括:波幅方程的增长,以及在准对规律方向上,一维结构的叠合.模式的选择由亚临界不稳定性机理确定,高分子薄膜的相对厚度在其中起着决定性的作用.
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出版历程
  • 收稿日期:  2011-01-17
  • 修回日期:  2011-05-24
  • 刊出日期:  2011-08-15

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