Sharan Surabhi, Gupta Prateek, Bahga Supreet Singh
Department of Mechanical Engineering, Indian Institute of Technology Delhi, Hauz Khas, New Delhi 110016, India.
School of Mechanical Engineering, Purdue University, West Lafayette, Indiana 47907, USA.
Phys Rev E. 2017 Feb;95(2-1):023103. doi: 10.1103/PhysRevE.95.023103. Epub 2017 Feb 2.
We describe the physical mechanism responsible for electrohydrodynamic (EHD) instability of a fluid layer with collinear conductivity gradient and electric field. In particular, we resolve the ambiguity in literature regarding the cause for switching between stationary and oscillatory modes of EHD instability. Using linear stability analysis, we show that a small perturbation in conductivity field perturbs the local electric field and also induces a perturbation charge. The coupling of base-state electric field with the perturbation charge leads to a force which causes overstability. Whereas, the coupling of base-state free charge with perturbation electric field leads to a force which causes EHD instability via a stationary mode. The proposed mechanism correctly explains the existence of stationary and oscillatory modes for varying conductivity gradients and wave number of disturbances, depending upon the relative magnitude of these two forces.
我们描述了具有共线电导率梯度和电场的流体层的电流体动力学(EHD)不稳定性的物理机制。特别地,我们解决了文献中关于EHD不稳定性的静止模式和振荡模式之间切换原因的模糊性。通过线性稳定性分析,我们表明电导率场中的小扰动会扰动局部电场并感应出扰动电荷。基态电场与扰动电荷的耦合产生一种导致过稳定性的力。而基态自由电荷与扰动电场的耦合产生一种通过静止模式导致EHD不稳定性的力。所提出的机制正确地解释了对于不同的电导率梯度和扰动波数,根据这两种力的相对大小,静止模式和振荡模式的存在。