Kelvin-Helmholtz instability in viscoelastic fluids in presence of electro-magnetic fields

被引:6
|
作者
Joshi, Amey S. [1 ]
Radhakrishna, M. C. [1 ]
Rudraiah, N. [2 ]
机构
[1] Bangalore Univ, Dept Phys, Bangalore 560056, Karnataka, India
[2] Bangalore Univ, Ctr Adv Studies Fluid Mech, Dept Math, Univ Grants Commiss, Bangalore 560056, Karnataka, India
关键词
dielectric liquids; electromagnetic fields; flow instability; magnetic fluids; non-Newtonian flow; non-Newtonian fluids; surface tension; viscoelasticity; viscosity; POTENTIAL FLOW-ANALYSIS; VORTEX SHEET; CAPILLARY INSTABILITY; MAGNETIC FLUIDS; SURFACE-TENSION; SINGULARITY; STABILITY; DYNAMICS; VISCOSITY; WAVES;
D O I
10.1063/1.3637033
中图分类号
O3 [力学];
学科分类号
08 ; 0801 ;
摘要
We investigate the root cause of Kelvin-Helmholtz instability with the aid of two simple models of energy exchange between the superposed fluids. We conclude that the density and surface tension of the fluids play a key role in determining the minimal relative speed that triggers the instability. We discuss the volume forces exerted by electric and magnetic field gradients on dielectric and ferro-fluids. We propose manipulating the field gradients to change the specific weight of fluids so that a flow of superposed fluids admits a greater relative velocity before the onset of Kelvin-Helmholtz instability. In order to include the effect of field gradients and viscosity in a closed form dispersion relation, we use the viscous potential flow approximation. It allows us to develop an analytical framework that works for dielectric fluids in presence of an electric field as well as ferro-fluid in presence of a magnetic field. The same framework is applicable to viscous as well as viscoelastic fluids described by the Oldroyd-B model. Our discussion of the Galilean transformation of the electromagnetic fields suggests ways to magnify the effects of field gradients. (C) 2011 American Institute of Physics. [doi: 10.1063/1.3637033]
引用
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页数:11
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