相关实验视频
Updated: Jul 4, 2025

Magnetically Induced Rotating Rayleigh-Taylor Instability
Published on: March 3, 2017
形态不稳定的动量传输在流体移位中随着粘度的变化而发生的变化
Takahiko Ban1, Hibiki Ishii1, Atsushi Onizuka1
1Division of Chemical Engineering, Department of Materials Engineering Science, Graduate School of Engineering Science, Osaka University, Machikaneyamacho 1-3, Toyonaka City, Osaka 560-8531, Japan. ban.takahiko.es@osaka-u.ac.jp.
萨夫曼-泰勒不稳定性通过热力学机制过渡到粘性指纹. 选择了产生较高的流量状态,澄清了物理化学转变点.
科学领域:
- 流体动力学 流体动力学
- 热力学是一种热力学.
- 复杂的系统复杂的系统.
背景情况:
- 萨夫曼-泰勒不稳定性显示了阶段性的不稳定形态,从稳定的接口过渡到粘性指纹和尖端分裂.
- 不稳定接口的非线性动力学受到流动特性的影响,但流动状态转换的物理化学机制尚不清楚.
研究的目的:
- 为了研究混合性位移中的界面不稳定性过渡背后的物理化学机制.
- 探索萨夫曼-泰勒不稳定性期间流量状态选择的热力学视角.
主要方法:
- 使用达西定律加上对流-扩散方程的数值分析.
- 计算动量传输和产生,以分析界面动态.
主要成果:
- 在可混合的位移中确定了流量依赖的流量状态转换.
- 证明在过渡过程中选择了具有更高产量的流量状态.
结论:
- 在萨夫曼-泰勒不稳定中,最大化产生的热力学原理支配了流量状态的选择.
- 这项研究阐明了确定粘性指纹现象中过渡点的物理化学机制.
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