Abstract

Deductive group symmetry treatment is applied to derive the similarity transformations for the free convective boundary layer flow of a class of non-Newtonian fluids past over a two-dimensional surface and flowing under the influence of transverse magnetic field. Numerical solutions are obtained for particular Non-Newtonian fluid model namely Prandtl Eyring fluid, in a graphical form . The important physical quantities like velocity distribution, skin friction coefficient and temperature variations are discussed.

Highlights

  • The classical theory of fluid mechanics is based upon the hypothesis of a linear relationship between two tensor components, shearing stress and rate of strain as, τ = −μ ∂u (1) ∂ yThe fluids with properties different from that described by equation (1), called Non-Newtonian fluids.Flow of Non-Newtonian fluids has attained a great success in the theory of fluid mechanics due to its applications in biological sciences and industry

  • In present work we concentrate our discussion on the similarity solution of steady laminar natural convection flows of generalized Non-Newtonian fluid

  • We investigate the MHD boundary layer flow of a class of Non-Newtonian fluids characterized by the property that its stress tensor component τij can be related to the strain rate component eij by the arbitrary continuous function of the type

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Summary

INTRODUCTION

In present work we concentrate our discussion on the similarity solution of steady laminar natural convection flows of generalized Non-Newtonian fluid. Such a class of fluids are severely omitted in the analysis due to mathematical complicity of its nonlinear stress-strain relationship. From these charts, we noticed that all the similarity solutions presented there in are derived either by adopting or by ad-hoc assumption on similarity variables. This method has been successfully applied to various non-linear problems by Abd-el-Malek et al [21], Adnan et al [22], Darji and Timol [23, 24]

GOVERNING EQUATIONS
SIMILARITY ANALYSIS
PRANDTL EYRING FLUID MODEL
RESULTS
CONCLUSION
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