2007
DOI: 10.1007/s00033-006-5117-4
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Exact self-similar solutions of the magnetohydrodynamic boundary layer system for power-law fluids

Abstract: In a particular self-similar case, the magnetohydrodynamic boundary layer system for an electrically conducting power-law fluid together with certain boundary conditions can be transformed into a boundary value problem for a third-order nonlinear ordinary differential equation, only whose (generalized) normal solutions possess the physical meaning of the original problem. Uniqueness, existence and nonexistence results are established for the problem. Representations are also given for all (generalized) normal … Show more

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Cited by 12 publications
(5 citation statements)
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References 15 publications
(18 reference statements)
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“…Mukhopadhyay et al [16] have investigated the problem of MHD boundary layer flow over a heated stretching sheet where the viscosity is considered to be variable. Zhang and Wang [17] have presented an exact selfsimilar solution for the problem of MHD boundary layer system for power-law fluids. Elbashbeshy et al [18] have considered the problem of unsteady laminar flow and heat transfer of an incompressible viscous fluid in the presence of thermal radiation, internal heat generation or absorbtion and magnetic field over an exponentially stretching surface subject to suction with an exponential temperature distribution.…”
Section: Introductionmentioning
confidence: 99%
“…Mukhopadhyay et al [16] have investigated the problem of MHD boundary layer flow over a heated stretching sheet where the viscosity is considered to be variable. Zhang and Wang [17] have presented an exact selfsimilar solution for the problem of MHD boundary layer system for power-law fluids. Elbashbeshy et al [18] have considered the problem of unsteady laminar flow and heat transfer of an incompressible viscous fluid in the presence of thermal radiation, internal heat generation or absorbtion and magnetic field over an exponentially stretching surface subject to suction with an exponential temperature distribution.…”
Section: Introductionmentioning
confidence: 99%
“…Here, B * shows the applied magnetic field which is a function of x and is in the form B � B 0 x (m− 1/2) , where B 0 denotes the uniform magnetic field (for precedence, we can see [48,49]), U * (x) denotes the free stream velocity and described in function of x, and is U * (x) � (u 0 /x − m ), in which u 0 is an invariable quantity and m (0 ≤ m ≤ 1) describes the Falkner Skan power law parameter. e expression β � β(2 − β) − 1 , in which β � (Ω/π) describes the Hartree pressure gradient.…”
Section: Mathematical Problems In Engineeringmentioning
confidence: 99%
“…The details of this phenomenon can be found in Davidson and applications can be found in petroleum industries, purification of crude oil, plasma physics, cooling of nuclear reactors, and aerodynamics . The first study on MHD boundary layer flows obeying a power‐law model was conducted by Sarpkaya and then followed by Zhang and Wang, Makinde, Makinde and Aziz, Makinde and Olanrewaju, and Khan et al They explored the same phenomenon under different boundary conditions and investigated the buoyancy effects on the thermal boundary layer over a vertical plate.…”
Section: Introductionmentioning
confidence: 99%