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E. Yariv
When an insulating particle is placed within a conducting liquid domain which is exposed to uniformly-applied electric and magnetic fields, a rotational Lorentz force density distribution is generated, thereby animating liquid flow. In this talk I will describe a series of theoretical investigations of this phenomenon. I will start my talk by describing the Stokes equations which govern the motion of viscous fluids, focusing upon their symmetry properties. I will then discuss flows driven by Lorentz force distribution, starting with the simplest case of spherical particles and following by more complicated non-isotropic configurations. These are analyzed by singular perturbation techniques such as slender-body theory and successive reflections.
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