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A general theoretical model for the magnetohydrodynamic flow of micropolar magnetic fluids. Application to Stokes flow

机译:微极性磁性流体的磁流体动力学流动的一般理论模型。在斯托克斯流中的应用

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Many practical applications, which have an inherent interest of physical and mathematical nature, involve the hydrodynamic flow in the presence of a magnetic field. Magnetic fluids comprise a novel class of engineering materials, where the coexistence of liquid and magnetic properties provides us with the opportunity to solve problems with high mathematical and technical complexity. Here, our purpose is to examine the micropolar magnetohydrodynamic flow of magnetic fluids by considering a colloidal suspension of ferromagnetic material (usually non-conductive) in a carrier magnetic liquid, which is in general electrically conductive. In this case, the ferromagnetic particles behave as rigid magnetic dipoles. Thus, the application of an external magnetic field, apart from the creation of an induced magnetic field of minor significance, will prevent the rotation of each particle, increasing the effective viscosity of the fluid and will cause the appearance of an additional magnetic pressure. Despite the fact that the general consideration consists of rigid particles of arbitrary shape, the assumption of spherical geometry is a very good approximation as a consequence of their small size. Our goal is to develop a general three-dimensional theoretical model that conforms to physical reality and at the same time permits the analytical investigation of the partial differential equations, which govern the micropolar hydrodynamic flow in such magnetic liquids. Furthermore, in the aim of establishing the consistency of our proposed model with the principles of both ferrohydrodynamics and magnetohydrodynamics, we take into account both magnetization and electrical conductivity of the fluid, respectively. Under this consideration, we perform an analytical treatment of these equations in order to obtain the three-dimensional effective viscosity and total pressure in terms of the velocity field, the total (applied and induced) magnetic field and the hydrodynamic and magnetic properties of the fluid, independently of the geometry of the flow. Moreover, we demonstrate the usefulness of our analytical approach by assuming a degenerate case of the aforementioned method, which is based on the reduction of the partial differential equations to a simpler shape that is similar to Stokes flow for the creeping motion of magnetic fluids. In view of this aim, we use the potential representation theory to construct a new complete and unique differential representation of magnetic Stokes flow, valid for non-axisymmetric geometries, which provides the velocity and total pressure fields in terms of easy-to-find potentials, via an analytical fashion.
机译:具有物理和数学性质的固有兴趣的许多实际应用涉及在存在磁场的情况下的流体动力学流动。磁性流体包括一类新颖的工程材料,液体和磁性的共存为我们提供了解决数学和技术复杂性高的问题的机会。在这里,我们的目的是通过考虑铁磁性材料(通常是非导电性)在通常为导电性的载磁性液体中的胶体悬浮液,来检查磁性流体的微极磁流体动力学流动。在这种情况下,铁磁粒子表现为刚性磁偶极子。因此,除了产生次要意义的感应磁场之外,施加外部磁场将防止每个粒子的旋转,增加流体的有效粘度,并且将引起额外的磁压力的出现。尽管通常考虑的因素是任意形状的刚性粒子,但由于球形几何尺寸小,因此假设球形几何形状非常好。我们的目标是开发一个符合物理现实的通用三维理论模型,同时允许对偏微分方程进行分析研究,该方程控制了这种磁性液体中的微极性流体动力学流动。此外,为了建立我们提出的模型与铁流体动力学和磁流体动力学原理的一致性,我们分别考虑了流体的磁化强度和电导率。在这种情况下,我们对这些方程式进行分析处理,以便获得三维有效粘度和总压力,包括速度场,总(施加和感应)磁场以及流体的流体力学和磁学性质。 ,与流的几何形状无关。此外,我们通过假设上述方法的简并性情况证明了我们的分析方法的有用性,该方法基于将偏微分方程简化为类似于斯托克斯流的简单形状,用于磁流体的蠕变运动。鉴于此目标,我们使用势能表示理论来构造新的磁斯托克斯流的完整且独特的微分表示,适用于非轴对称几何形状,从而以易于发现的势能提供速度和总压力场,通过分析的方式。

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