4.0 Article

Numerical Simulation of MHD Stagnation Point Flow of Micropolar Heat Generating and Dissipative Nanofluid : SLM Approach

Publisher

NATL ACAD SCIENCES INDIA
DOI: 10.1007/s40010-020-00704-x

Keywords

Micropolar nanofluid; Stagnation point flow; Viscous dissipation; Joule heating; Thermophoretic and Brownian diffusions; Successive linearization method (SLM)

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This paper investigates the magnetohydrodynamic stagnation point flow of a micropolar nanofluid influenced by heat generation and viscous dissipation. Nonlinear ordinary differential equations are solved using the successive linearization method, and the effects of various dimensionless parameters on the flow field are discussed. Results show that temperature distribution gradually increases with the rise of heat generation and microrotation parameters.
In the present paper, we study the magnetohydrodynamic stagnation point flow dealing with heat and mass transfer of a micropolar nanofluid influenced with heat generation and viscous dissipation. Nonlinear ordinary differential equations are obtained by applying suitable similarity transformation on the governing partial differential equations. These differential equations have been solved by successive linearization method (SLM). The effects of various dimensionless parameters, such as heat generation parameter, thermophoretic parameter and stagnation parameter on the flow field, are discussed through tables and graphs by accumulating sufficient data using SLM. Results show many important facts, including temperature distribution gradual increment with the increase of heat generation and microrotation parameters. Quadratic multiple regression analysis has been performed for skin friction coefficient, local Sherwood number and local Nusselt number. When free stream velocity and stretching velocity are equal, variation in microrotation and magnetic field leads to very low perturbation in skin friction, local Sherwood number and local Nusselt number, whereas when free stream velocity is dominant over stretching velocity, there occurs reverse heat flow at the surface of the sheet.

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