Viscous dissipation and Joule heating in case of variable electrical conductivity Carreau–Yasuda nanofluid flow in a complex wavy asymmetric channel through porous media

Sameh E. Ahmed, A. Arafa, Sameh A. Hussein
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Abstract

This paper focuses on flow structures and thermal fields of the Carreau–Yasuda (CY) nanofluid model through a two-dimensional, wavy, complicated vertical asymmetrical conduit filled with porous elements. Formulations of the viscous dissipation in the case of CY nanofluids are derived and nonlinear radiation flux as well as joule heating are examined. Buongiorno’s nanofluid approach, which involves Brownian motion and thermophoresis aspects is considered. The electrical conductivity of the suspension is considered as a variable where it depends upon the ambient temperature and concentration distributions and the Joule heating impacts are not neglected. The approach of solving the problem is contingent upon converting the system to dimensionless form then the lubrication approach with low magnetic Reynold numbers is applied. Numerical solutions are found for the resultant system, and wide ranges are considered for Weissenberg number We, non-Newtonian parameter n and Darcy number [Formula: see text], namely, [Formula: see text], [Formula: see text] and [Formula: see text], respectively. The major results indicated that gradients of the pressure are higher in case of shear thickening [Formula: see text] comparing to in the instance of shear thinning [Formula: see text]. Also, the velocity is enhanced, close to the channel’s lowest portion, as the Weissenberg number is growing. The variable electrical conductivity gives a higher mass transfer rate compared to the constant property.
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导电率可变的 Carreau-Yasuda 纳米流体在穿过多孔介质的复杂波浪形非对称通道中流动时的粘性耗散和焦耳热
本文重点研究了 Carreau-Yasuda (CY) 纳米流体模型在充满多孔元素的二维波浪形复杂垂直不对称导管中的流动结构和热场。推导了 CY 纳米流体的粘性耗散公式,并研究了非线性辐射通量和焦耳热。考虑了 Buongiorno 的纳米流体方法,其中涉及布朗运动和热泳方面。悬浮液的导电率被视为一个变量,它取决于环境温度和浓度分布,焦耳热的影响也没有被忽略。解决问题的方法取决于将系统转换为无量纲形式,然后应用低磁雷诺数的润滑方法。对结果系统进行了数值求解,并考虑了魏森伯格数 We、非牛顿参数 n 和达西数[公式:见正文]的宽范围,即分别为[公式:见正文]、[公式:见正文]和[公式:见正文]。主要结果表明,与剪切变稀[式:见正文]的情况相比,剪切变稠[式:见正文]的情况下压力梯度更大。此外,随着魏森伯格数的增加,靠近通道最低部分的速度也会增加。与恒定电导率相比,可变电导率的传质速率更高。
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