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Flow control of magnetic fluids exposed to magnetic fields

机译:暴露于磁场的磁流体的流量控制

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摘要

The description of flow in ferrohydrodynamics (Rosensweig, 1985) is based on a combination of equations, namely the continuity equation, the Navier-Stokes equation, the Maxwell equations and particular equations for the magnetization. Since the different models to describe the relaxation of magnetization differ, the adequate one has yet to be identified. By comparing experimental and simulation data of a model system, this goal may get achieved. As a model system, a Taylor-Couette apparatus was chosen. In this paper, experimental results concerning the transition form circular Couette flow to Taylor vortex flow at different field strengths of an axial magnetic field are compared to a linear stability analysis. The relaxation equation established by Shliomis (Shliomis, 1972) and the Debye-Model with a field dependent relaxation time showed to give qualitative accordance with the experimental data.
机译:铁流体动力学(Rosensweig,1985)的流动描述基于方程式的组合,即连续性方程,Navier-Stokes方程,麦克风方程和用于磁化的特定方程。由于描述了磁化放松的不同模型不同,因此尚未识别了足够的。通过比较模型系统的实验和仿真数据,可以实现这一目标。作为模型系统,选择了泰勒 - 圆饼装置。在本文中,与线性稳定性分析进行了比较了关于轴向磁场的不同场强的圆形耦合到圆锥涡流的圆形耦合流的实验结果。由Shliomis(Shliomis,1972)建立的弛豫方程和具有田间依赖性弛豫时间的德拜模型表示根据实验数据进行定性。

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