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On radiative heat transfer in stagnation point flow of MHD Carreau fluid over a stretched surface

机译:关于MHD Carreau流体在拉伸表面上的驻点流中的辐射传热

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This paper investigates the behavior of MHD stagnation point flow of Carreau fluid in the presence of infinite shear rate viscosity. Additionally heat transfer analysis in the existence of non-linear radiation with convective boundary condition is performed. Moreover effects of Joule heating is observed and mathematical analysis is presented in the presence of viscous dissipation. The suitable transformations are employed to alter the leading partial differential equations to a set of ordinary differential equations. The subsequent non-straight common ordinary differential equations are solved numerically by an effective numerical approach specifically Runge-Kutta Fehlberg method alongside shooting technique. It is found that the higher values of Hartmann numberMcorrespond to thickening of the thermal and thinning of momentum boundary layer thickness. The analysis further reveals that the fluid velocity is diminished by increasing the viscosity ratio parameter(β?)and opposite trend is observed for temperature profile for both hydrodynamic and hydromagnetic flows. In addition the momentum boundary layer thickness is increased with velocity ratio parameterαand opposite is true for thermal boundary layer thickness.
机译:本文研究了无限剪切速率粘度存在下Carreau流体MHD停滞点流动的行为。另外,在存在具有对流边界条件的非线性辐射的情况下进行传热分析。此外,观察到焦耳加热的影响,并且在存在粘性耗散的情况下进行了数学分析。采用适当的变换将前导的偏微分方程改变为一组常微分方程。通过有效的数值方法,特别是Runge-Kutta Fehlberg方法以及射击技术,可以对随后的非直线常微分方程进行数值求解。发现哈特曼数的较高值对应于热的增厚和动量边界层厚度的减薄。分析还揭示出,通过增加粘度比参数(β1)降低了流体速度,并且在流体动力学和流体电磁流动的温度分布中观察到相反的趋势。此外,动量边界层的厚度随速度比参数α的增加而增加,而热边界层的厚度则相反。

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