On the solution of MHD Jeffery–Hamel problem involving flow between two nonparallel plates with a blood flow application

IF 2.8 Q2 THERMODYNAMICS Heat Transfer Pub Date : 2024-05-02 DOI:10.1002/htj.23064
Atallah El-Shenawy, Mohamed El-Gamel, Mahmoud Abd El-Hady
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Abstract

The Jeffery–Hamel flow phenomenon appears in a variety of real-world applications involving the flow of two nonparallel plates. BY using a similarity transformation derived from the equation of continuity, partial differential equations determining flow characteristics are translated into nonlinear ordinary differential equations. The problem involves the flow of a specific type of fluid, namely, an incompressible and electrically conducting fluid, between two nonparallel plates. The flow is assumed to be steady, two-dimensional, and subject to certain boundary conditions. Specifically, the plates are impermeable, and the fluid adheres to a no-slip condition, resulting in zero fluid velocity at the plates' surfaces. Moreover, the problem incorporates the effects of magnetic fields and pressure fluctuations, making it highly applicable to scenarios, such as blood flow through arteries in the human body, which can be modeled as a special case of the magnetohydrodynamic (MHD) Jeffery–Hamel problem referred to as the (MHD) blood pressure equation. This work compares two numerical approaches for solving the MHDs Jeffery–Hamel problem: B-spline and Bernstein polynomial collocation. The given approaches are used to discretize and transform the equation into a system of algebraic equations. Matrix algebra techniques are then used to solve the resultant system. A complete error analysis and convergence rates for different grid sizes are derived for both methods and are used to compare the accuracy and efficiency of the two approaches. Both approaches produce correct solutions, according to the numerical findings, although the Bernstein polynomial collocation method is more efficient and accurate than the B-spline collocation.

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关于涉及两块非平行板之间流动的 MHD 杰弗里-哈梅尔问题的求解,以及血液流动的应用
杰弗里-哈梅尔流动现象出现在涉及两个非平行板流动的各种实际应用中。通过使用从连续性方程导出的相似性变换,决定流动特性的偏微分方程被转化为非线性常微分方程。问题涉及一种特定类型的流体,即不可压缩的导电流体,在两块不平行板之间的流动。假定流动是稳定的、二维的,并受某些边界条件的限制。具体来说,板是不可渗透的,流体遵守无滑动条件,导致板表面的流体速度为零。此外,该问题还包含磁场和压力波动的影响,因此非常适用于人体动脉血流等情况,可作为磁流体力学(MHD)杰弗里-哈梅尔问题的特例进行建模,称为(MHD)血压方程。本研究比较了两种解决 MHD 杰弗里-哈梅尔问题的数值方法:B-样条曲线和伯恩斯坦多项式配置。给出的方法用于将方程离散化并转化为代数方程系统。然后使用矩阵代数技术求解结果系统。两种方法都得出了完整的误差分析和不同网格大小的收敛率,并用于比较两种方法的精度和效率。根据数值结果,两种方法都能得出正确的解,但伯恩斯坦多项式配位法比 B-样条曲线配位法更有效、更准确。
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来源期刊
Heat Transfer
Heat Transfer THERMODYNAMICS-
CiteScore
6.30
自引率
19.40%
发文量
342
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