Results 1 to 10 of about 37 (36)
Non-stationary Navier–Stokes equations in 2D power cusp domain
Advances in Nonlinear Analysis, 2021 The initial boundary value problem for the non-stationary Navier-Stokes equations is studied in 2D bounded domain with a power cusp singular point O on the boundary. We consider the case where the boundary value has a nonzero flux over the boundary.
Pileckas Konstantin, Raciene Alicija
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Scaling invariance theory and numerical transformation method: A unifying framework
Applications in Engineering Science, 2020 In a transformation method, the numerical solution of a given boundary value problem is obtained by solving one or more related initial value problems. Therefore, a transformation method, like a shooting method, is an initial value method.
Riccardo Fazio
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Free convection flow of conducting micropolar fluid with thermal relaxation including heat sources
Journal of Applied Mathematics, Volume 2004, Issue 4, Page 271-292, 2004., 2004 The present work is concerned with unsteady free convection flow of an incompressible electrically conducting micropolar fluid, bounded by an infinite vertical plane surface of constant temperature. A uniform magnetic field acts perpendicularly to the plane.
Magdy A. Ezzat
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Journal of Applied Mathematics, Volume 2003, Issue 2, Page 65-86, 2003., 2003 An analysis is performed to study radiation effects on magnetohydrodynamic (MHD) unsteady free‐convection flow past a semi‐infinite vertical plate with variable surface temperature in the presence of transversal uniform magnetic field. The boundary layer equations are transformed into a linear algebraic system by an implicit finite‐difference method. A
M. A. Abd El-Naby +2 more
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Journal of Applied Mathematics, Volume 2, Issue 2, Page 93-103, 2002., 2002 We investigate the problem of free convection heat transfer near an isothermal stretching sheet. This has been done under the simultaneous action of buoyancy, radiation, and transverse magnetic field. The governing equations are solved by the shooting method.
Ahmed Y. Ghaly, Elsayed M. E. Elbarbary
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The effect of Coriolis force on nonlinear convection in a porous medium
International Journal of Mathematics and Mathematical Sciences, Volume 17, Issue 3, Page 515-536, 1994., 1994 Nonlinear convection in a porous medium and rotating about vertical axis is studied in this paper. An upper bound to the heat flux is calculated by the method initiated first by Howard [6] for the case of infinite Prandtl number. For Ta ≪ 0(1), the rotational effect is not significant.
D. H. Riahi
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International Journal of Mathematics and Mathematical Sciences, Volume 15, Issue 4, Page 789-794, 1992., 1991 The Darcy‐Brinkman free convection near a wedge and a cone in a porous medium with high porosity has been considered. The surfaces are subjected to a mixed thermal boundary condition characterized by a parameter m; m = 0, 1, ∞ correspond to the cases of prescribed temperature, prescribed heat flux and prescribed heat transfer coefficient respectively ...
G. Ramanaiah, V. Kumaran
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Boundary layer analysis of nonlinear reaction-diffusion equations in a smooth domain
Advances in Nonlinear Analysis, 2017 In this article, we consider a singularly perturbed nonlinear reaction-diffusion equation whose solutions display thin boundary layers near the boundary of the domain.
Jung Chang-Yeol +2 more
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Shear flow past a flat plate in hydromagnetics
International Journal of Mathematics and Mathematical Sciences, Volume 3, Issue 3, Page 521-534, 1980., 1979 The problem of simple shear flow past a flat plate has been extended to the hydromagnetic case in which a viscous, electrically conducting, incompressible fluid flows past an electrically insulated flat plate with a magnetic field parallel to the plate. For simplicity all physical parameters are assumed constant.
S. R. N. Sastry
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Global inviscid limit of 2D, stationary Navier-Stokes and stability of Prandtl expansions
Forum of Mathematics, PiIn this work, we establish the convergence of 2D, stationary Navier-Stokes flows with viscosity $\varepsilon> 0$ , $(u^\varepsilon , v^\varepsilon )$ to the classical Prandtl boundary layer, $(\bar {u}_p, \bar {v}_p)$ , posed on the ...
Sameer Iyer, Nader Masmoudi
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