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Effect of normal and parallel magnetic fields on the stability of interfacial flows of magnetic fluids in channels

机译:正,平行磁场对通道中磁性流体界面流动稳定性的影响

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摘要

The effect of an imposed magnetic field on the linear stability of immiscible two-fluid Poiseuille flow in a channel is examined for low Reynolds numbers. Surface tension acts on the interface, the fluids have different densities and viscosities, and one fluid is magnetic (ferrofluid). A Langevin function is used to model the fluid magnetization, resulting in a nonlinear permeability; the stability properties depend on this permeability relation both directly and indirectly, through the base state solution. Uniform magnetic fields applied normal or parallel to the interface both lead to an interfacial instability. Normal fields excite longer wavelength modes, generally having higher growth rates, but parallel fields can excite faster growing modes in high permeability fluids at large applied field strength. Whether or not the field stabilizes or destabilizes the flow depends on the viscosity and layer thickness ratios in a simple way, while the placement of the magnetic fluid layer does not play a major role. Growth rates predicted for realistic microchannel conditions are shown to be large enough to make ferrofluid manipulation a practical method of control.
机译:对于低雷诺数,检查了施加的磁场对通道中不可混溶的二流体泊瓦伊流动的线性稳定性的影响。表面张力作用在界面上,流体的密度和粘度不同,一种流体是磁性的(铁磁流体)。 Langevin函数用于对流体磁化建模,从而导致非线性磁导率;通过基态解,稳定性直接或间接地取决于该渗透率关系。垂直或平行于界面施加的均匀磁场都会导致界面不稳定。正场激发较长的波长模式,通常具有较高的生长速率,但平行场可以在高施加场强的高渗透率流体中激发较快的生长模式。磁场是否使流量稳定或不稳定,以简单的方式取决于粘度和层厚比,而磁性流体层的放置则不起主要作用。现实的微通道条件下预测的增长率显示出足够大,以使铁磁流体操纵成为一种实用的控制方法。

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