硅纳米流体在拉伸圆柱体上的非稳态流动,以及不同形状的纳米颗粒和焦耳加热的影响

Pub Date : 2024-07-12 DOI:10.24425/ather.2024.151222
R. Ali, Azhar Iqbal, Tasawar Abbass, Touqeer Arshad, Azeem Shahzad
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引用次数: 0

摘要

事实上,纳米流体因其众多优点和潜在应用而在各个领域备受关注。特别是二氧化硅纳米流体,其吸引力在于制备成本低、生产工艺简单、化学性质可控、环境安全以及在基液中均匀悬浮的特殊能力,这使其成为各种应用的理想候选材料。在本研究中,我们研究了水基二氧化硅纳米流体在连续磁场作用下通过拉伸圆柱体时的流动分析,包括焦耳加热效应。研究涉及数学模型的开发和以偏微分方程表示的控制方程的制定。随后通过适当的变换将这些方程转化为非线性常微分方程。为了获得数值解,使用了 MATLAB bvp4c 求解器技术。研究探讨了无量纲参数对速度和热分布的影响。研究发现,速度分布 f'(η) 与体积分数 ϕ 呈直接关系,与不稳定性参数 S 和磁性参数 M 呈反比关系,温度分布 θ(η) 随着 ϕ 和 M 以及埃克特数的增加而增强。然而,它随着 S 和普朗特数的增加而减小。表中显示了局部努塞尔特数和表皮摩擦的结果。
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Unsteady flow of silica nanofluid over a stretching cylinder with effects of different shapes of nanoparticles and Joule heating
Indeed, nanofluids have garnered significant interest in various fields due to their numerous advantages and potential ap-plications. The appeal of SiO2 nanofluid, in particular, lies in its low preparation cost, simple production process, controlled chemistry, environmental safety and its exceptional ability to be homogeneously suspended in the base fluid, which makes it a promising candidate for a variety of applications. In this study, we investigate the flow analysis of a water based silicon dioxide nanofluid, passing over a stretched cylinder while subjected to a continuous magnetic field, including Joule heating effects. The research involves the development of a mathematical model and the formulation of governing equations rep-resented as partial differential equations. These equations are subsequently transformed into non-linear ordinary differential equations through suitable transformations. To obtain a numerical solution, the MATLAB bvp4c solver technique is em-ployed. The study investigates the implications of dimensionless parameters on velocity and thermal distributions. It is observed that the velocity distribution f'(η) exhibits a direct relationship with the volumetric fraction ϕ and an inverse relationship with the unsteadiness parameter S, the magnetic parameter M, and the temperature distribution θ(η) shows an enhancement for the increasing ϕ and M, as well as the Eckert number. However, it declines against S and the Prandtl number. The results for local Nusselt number and skin frictions are depicted in Tables.
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