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Radiation effects on MHD flow through porous media

K Pr Pr −1 Sc −1 h =M* +d,G1 = PGr −r 1,G2 = SGcthe oscillatory flow an infinite vertical porous, plate with constant suction

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Numerical/Laplace transform analysis for MHD

suction and heat source in slip-flow regime wereTaylors series to expand T4 about the free tÞ ¼ t À 1 þ 2g2ScÁerfcgp

Effects of variable viscosity, heat and mass transfer on

ISSN 1819-6608 ψ= 2Uνx 1+ m f ( x,η ) (7) η= y (1+ m)U 2νx (8) The viscosity is assumed to be an inverse

Thermal radiation on linearly accelerated vertical plate with

Then under usual Boussinesqs approximation the 1 0.8 C 0.6 0.4 Sc = 0.16 Sc = 0.3porous medium with constant suction and heat flux

Effects of variable viscosity, heat and mass transfer on

ISSN 1819-6608 ψ= 2Uνx 1+ m f ( x,η ) (7) η= y (1+ m)U 2νx (8) The viscosity is assumed to be an inverse

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Magnetic field effect on a three-dimensional mixed convective

The transverse sinusoidal suction velocity is taken as follows: ( )vw z = −V0 ⎡ ⎢1 ⎣ + ε Cos πz L ⎤ ⎥ ⎦ (7) 119 Ahmed

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Magnetic field effect on a three-dimensional mixed convective

The transverse sinusoidal suction velocity is taken as follows: ( )vw z = −V0 ⎡ ⎢1 ⎣ + ε Cos πz L ⎤ ⎥ ⎦ (7) 119 Ahmed

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Chebyshev finite difference method for the effects

þ 1 n À n þ 2Pr f h0 ¼ 0 /00 À 4Sc f 0/ þ 2Sc f /0 À 4cSc Re/ ¼ 0 ð12Þ ð13Þ ð14Þ 64 A

Thermal radiation on linearly accelerated vertical plate with

Then under usual Boussinesqs approximation the 1 0.8 C 0.6 0.4 Sc = 0.16 Sc = 0.3porous medium with constant suction and heat flux