Thermophysical analysis of three‐dimensional magnetohydrodynamic flow of a tangent hyperbolic nanofluid

In this article, we use the Buongiorno model to study the three‐dimensional tangent hyperbolic nanofluid flow over a stretched sheet. The study investigates the impact of velocity slip on the flow and heat transfer features in a tangent hyperbolic nanofluid. For a better fit with experimental observ...

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Veröffentlicht in:Engineering reports (Hoboken, N.J.) N.J.), 2020-04, Vol.2 (4), p.n/a
Hauptverfasser: Oyelakin, Ibukun S., Lalramneihmawii, PC, Mondal, Sabyasachi, Nandy, Samir K., Sibanda, Precious
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Sprache:eng
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Zusammenfassung:In this article, we use the Buongiorno model to study the three‐dimensional tangent hyperbolic nanofluid flow over a stretched sheet. The study investigates the impact of velocity slip on the flow and heat transfer features in a tangent hyperbolic nanofluid. For a better fit with experimental observations. We assume that the nanoparticle mass flux at the boundary is zero as opposed to a prescribed concentration at the surface. Using appropriate transformations, we reduce the partial differential equations that describe the momentum, energy, and concentration transport to ordinary differential equations. Numerical solutions of the equations are obtained using the spectral method. Graphical illustration of the physical influence of various parameters on the flow features, the skin friction coefficient, and the local Nusselt number is given. The results indicate, that particle Brownian motion has a negligible impact on the rate of heat transfer. The impact of the modified Weissenberg number, a measure of the ratio of elastic to viscous forces, causes a reduction in the fluid velocity. The results are shown to be good agreement with those in related studies in the literature. The three‐dimensional flow of a tangent hyperbolic nanofluid over a stretching sheet is formulated using the Buongiorno's model. The study investigates the impact of velocity slip on the heat and mass transfer characteristics of a tangent hyperbolic nanofluid. In addition, we assume that the nanoparticle mass flux at the surface is zero so as to have a better reflection of experimental reality as opposed to a fixed concentration at the surface.
ISSN:2577-8196
2577-8196
DOI:10.1002/eng2.12144