Exact solutions for the description of nonuniform unidirectional flows of magnetic fluids in the Lin–Sidorov–Aristov class

L. Goruleva, E. Prosviryakov
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Abstract

The paper considers the exact integration of magnetic hydrodynamic equations for describing nonuniform unidirectional flows of viscous incompressible fluids. The construction of an exact solution is based on the well-known representation of hydrodynamic fields as the Lin–Sidorov–Aristov class. The 3d magnetic field is described by linear forms with respect to two spatial coordinates (longitudinal, or horizontal). The coefficients of the linear forms depend on the third coordinate and time. In view of the incompressibility condition, the 1D velocity field depends on two coordinates and time. The pressure is shown to be determined by a quadratic form with constant coefficients. These coefficients are determined by pressure distribution on the known (free) boundary. The exact solution is illustrated by the integration of non-1D hydrodynamic fields in the case of the steady motion of a conducting viscous incompressible fluid. This solution is polynomial, and it will be useful for the formulation of new problems of hydrodynamic stability.
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描述林-西多罗夫-阿里斯托夫类磁性流体非均匀单向流动的精确解
本文研究了描述粘性不可压缩流体非均匀单向流动的磁性流体力学方程的精确积分问题。精确解的构建基于著名的流体动力场表示法 Lin-Sidorov-Aristov 类。三维磁场由两个空间坐标(纵向或横向)的线性形式描述。线性形式的系数取决于第三个坐标和时间。鉴于不可压缩性条件,一维速度场取决于两个坐标和时间。压力由具有常数系数的二次方形式决定。这些系数由已知(自由)边界上的压力分布决定。在导电粘性不可压缩流体稳定运动的情况下,通过对非一维流体动力场进行积分,说明了精确解法。这个解是多项式的,它将有助于提出新的流体力学稳定性问题。
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