A study on the pressure-driven flow of magnetized non-Newtonian Casson fluid between two corrugated curved walls of an arbitrary phase difference

IF 2.8 Q2 THERMODYNAMICS
Heat Transfer Pub Date : 2024-08-07 DOI:10.1002/htj.23146
Maham Mujahid, Zaheer Abbas, Muhammad Yousuf Rafiq
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Abstract

Pressure-driven movement is a fundamental concept with numerous applications in various industries, scientific disciplines, and fields of engineering. Its proper execution is vital for promoting revolutionary innovations and providing solutions in numerous sectors. Therefore, this article scrutinizes the pressure-driven flow of magnetized Casson fluid between two curved corrugated walls. The geometry of the channel is represented mathematically in an orthogonal curvilinear coordinate system. The corrugation grooves are described by sinusoidal functions with phase differences between the corrugated curved walls. The boundary perturbation method is used to find the analytical solution for the velocity field and volumetric flow rate, taking the corrugation amplitude as the perturbation parameter. The results show that the peak of the velocity increases with the radius of curvature and the width of the channel for a constant pressure gradient. The velocity exhibited a declining trend due to an increase in the Casson fluid parameter. For a sufficiently large corrugation wavenumber, the flow rate decreases, and the phase difference becomes irrelevant. However, the reduction in flow can be minimized by decreasing the channel radius of curvature. In general, a smooth curved channel will give the maximum flow rate for a large corrugation wavenumber. The model can be used to simulate blood flow in arteries with varying geometries and magnetic fields, aiding in the study of cardiovascular diseases and the design of medical devices like stents.

关于磁化非牛顿卡松流体在任意相位差的两波纹曲壁之间的压力驱动流动的研究
压力驱动运动是一个基本概念,在各行各业、科学学科和工程领域都有大量应用。它的正确执行对于促进革命性创新和为众多领域提供解决方案至关重要。因此,本文仔细研究了磁化卡松流体在两个弯曲波纹壁之间的压力驱动流动。通道的几何形状在正交曲线坐标系中以数学方式表示。波纹槽由正弦函数描述,波纹曲壁之间存在相位差。以波纹振幅作为扰动参数,采用边界扰动法求得速度场和容积流量的解析解。结果表明,在压力梯度不变的情况下,速度峰值随曲率半径和通道宽度的增加而增加。由于卡松流体参数的增加,速度呈下降趋势。对于足够大的波纹波数,流速会降低,相位差变得无关紧要。不过,可以通过减小通道曲率半径来尽量减少流量的减少。一般来说,在波纹波数较大的情况下,光滑的弯曲通道会产生最大流速。该模型可用于模拟不同几何形状和磁场的动脉血流,有助于心血管疾病的研究和支架等医疗设备的设计。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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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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