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Jump momentum boundary condition at a fluid-porous dividing surface: Derivation of the closure problem

机译:流体多孔分隔面上的跳跃动量边界条件:闭合问题的推导

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The method of volume averaging is used to derive a stress jump boundary condition that takes the form epsilon(-1)(beta omega) partial derivative (omega)/partial derivative y - partial derivative (eta)/partial derivative y = Kappa(-1)/a(nu s) (omega). Here K-1 is the tangential component of a mixed stress tensor which combines the global and Brinkman stresses at the dividing surface. The computation of the Brinkman stress at the boundary is carried out by using polynomial functions describing the spatial changes of the porosity. Local closure problems are derived for the determination of the global stress contribution at the inter-region. At this stage, an alternative methodology is proposed in order to estimate the mixed stress tensor, which has been related to the stress jump coefficient proposed in the literature. Results for the jump coefficient are found to be in good agreement with previous calculations. (c) 2007-Elsevier Ltd. All rights reserved.
机译:体积平均法用于导出应力跃变边界条件,其形式为epsilon(-1)βbeta偏导数Ω/偏导数y-偏导数η /偏导数y = Kappa(-1)/ a(nu s)(ω)。在这里,K-1是混合应力张量的切向分量,它在分界面处结合了整体应力和布林克曼应力。边界处的布林克曼应力的计算是通过使用描述孔隙度空间变化的多项式函数进行的。为了确定区域间的整体压力贡献,导出了局部封闭问题。在这一阶段,为了估计混合应力张量,提出了另一种方法,该方法与文献中提出的应力跃变系数有关。发现跳跃系数的结果与先前的计算非常吻合。 (c)2007-Elsevier Ltd.保留所有权利。

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