Abstract
Due to their unique microstructures, micropolar fluids have attracted enormous attention for their industrial applications, including convective heat and mass transfer polymer production and rigid and random cooling particles of metallic sheets. The thermodynamical demonstration is an integral asset for anticipating the ideal softening of heat transfer. This is because there is a decent connection between mathematical and scientific heat transfers through thermodynamic anticipated outcomes. A model is developed under the micropolar stream of a non-Newtonian (3rd grade) liquid in light of specific presumptions. Such a model is dealt with by summoning likeness answers for administering conditions. The acquired arrangement of nonlinear conditions is mathematically settled using the fourth-fifth order Runge-Kutta-Fehlberg strategy. The outcomes of recognized boundaries on liquid streams are investigated in subtleties through the sketched realistic images. Actual amounts like Nusselt number, Sherwood number, and skin-part coefficient are explored mathematically by tables. It is observed that the velocity distribution boosts for larger values of any of
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\begin{document}$$\alpha _1$$\end{document}
α
1
,
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\begin{document}$$\beta$$\end{document}
β
, and declines for larger
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2
and Hartmann numbers. Furthermore, the temperature distribution
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\begin{document}$$\theta (\eta )$$\end{document}
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(
η
)
shows direct behavior with the radiation parameter and Eckert number, while, opposite behavior with
Pr
, and
K
. Moreover, the concentration distribution shows diminishing behavior as we put the higher value of the Brownian motion number.