4.3 Article

Impact of surface temperature and convective boundary conditions on a Nanofluid flow over a radially stretched Riga plate

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SAGE PUBLICATIONS LTD
DOI: 10.1177/09544089211054407

Keywords

Radially stretched Riga sheet; prescribed surface temperature; prescribed surface concentration (PSC); zero mass flux concentration

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This study provides an optimal homotopic analytical methodology for the steady circulation over a non-isothermal radially stretched Riga disc unit. Various boundary conditions and parameters are considered to analyze the heat and mass transfer processes. The model shows that the modified Hartman number improves velocity distribution and reduces temperature distribution.
The current work provides the optimal homotopic analytical methodology for the steady circulation over a non-isothermal radially stretched Riga plate/disc unit. The attributes of the heat, along with the mass transfer process, are assessed in the existence of variable transport and magnetic features. Radial stretched Riga disc is considered along with additional realistic boundary heating conditions, namely, prescribed surface temperature as well as prescribed surface concentration, convective boundary conditions and also zero mass flux concentration on the surface area of the Riga disc. The model tracks Brownian motion as well as the thermal diffusion of nanoparticles in fluid circulation all at once. Regulating equations, which are highly coupled, are changed right into non-dimensional equations using appropriate transformations of similarity. Through assembling series solutions, the resulting framework is planned and examined. Graphic summaries are offered for the rheological qualities of various parameters in size for velocity, temperature, as well as nanoparticles. The modified Hartman number improves the velocity distribution and reduces the temperature distribution in both prescribed surface temperature and convective boundary condition cases. The effect of the chemical reaction parameter shows the reduced concentration distribution for the prescribed surface temperature case. In contrast, it is precisely the opposite in the convective boundary condition case.

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