The effect of the ratio (the strain retardation time to the sress relaxation time) on magneto-hydrodynamic viscoelastic fluid (Walters ’ lquid B’) layer heated From below confined between tow horizontal planes has been studied. Linear stability theory and normal mode analysis are used to derive an differential equation of sixth order, and an exact solution for natural instability is obtained.Critical Rayleigh numbers and wave numbers for the onset of instability are discussed graphically as functions of , the Chandrasekhar number for various values of the Fourier number, and relaxation time at a constant value for Prandtl number
The coupled thermogravitational and thermocapillary instability in a thin fluid layer of a viscoelas...
In this paper, the linear stability of a saturated rotating porous layer of viscoelastic fluid which...
Magnetohydrodynamic convection (MHD convection) in a horizontal porous-layer filled by a plasma, imb...
AbstractOverstability in a horizontal layer of a viscoelastic fluid is considered in the presence of...
AbstractOverstability in a horizontal layer of a viscoelastic fluid is considered in the presence of...
The thermal instability of a rotating Rivlin-Ericksen viscoelastic fluid in the presence of uniform ...
The thermal instability of a rotating Rivlin-Ericksen viscoelastic fluid in the presence of uniform ...
This paper is devoted to an examination of the stability of a horizontal layer of fluid heated below...
The instability of a viscoelastic fluid saturating a horizontal porous layer heated from below is st...
The stability of a viscoelastic fluid in a densely packed horizontal porous layer heated from below ...
Two constitutive equations for viscoelastic fluids are examined in linearized hydrodynamic stability...
The stability of a viscoelastic fluid in a densely packed horizontal porous layer heated from below ...
The stability of a viscoelastic fluid in a densely packed horizontal porous layer heated from below ...
The theory described in an earlier paper (Chandrasekhar 1953 b) is extended in a manner which enable...
Thermal instability in a horizontal layer of Walter’s B' visco-elastic nanofluid has been investigat...
The coupled thermogravitational and thermocapillary instability in a thin fluid layer of a viscoelas...
In this paper, the linear stability of a saturated rotating porous layer of viscoelastic fluid which...
Magnetohydrodynamic convection (MHD convection) in a horizontal porous-layer filled by a plasma, imb...
AbstractOverstability in a horizontal layer of a viscoelastic fluid is considered in the presence of...
AbstractOverstability in a horizontal layer of a viscoelastic fluid is considered in the presence of...
The thermal instability of a rotating Rivlin-Ericksen viscoelastic fluid in the presence of uniform ...
The thermal instability of a rotating Rivlin-Ericksen viscoelastic fluid in the presence of uniform ...
This paper is devoted to an examination of the stability of a horizontal layer of fluid heated below...
The instability of a viscoelastic fluid saturating a horizontal porous layer heated from below is st...
The stability of a viscoelastic fluid in a densely packed horizontal porous layer heated from below ...
Two constitutive equations for viscoelastic fluids are examined in linearized hydrodynamic stability...
The stability of a viscoelastic fluid in a densely packed horizontal porous layer heated from below ...
The stability of a viscoelastic fluid in a densely packed horizontal porous layer heated from below ...
The theory described in an earlier paper (Chandrasekhar 1953 b) is extended in a manner which enable...
Thermal instability in a horizontal layer of Walter’s B' visco-elastic nanofluid has been investigat...
The coupled thermogravitational and thermocapillary instability in a thin fluid layer of a viscoelas...
In this paper, the linear stability of a saturated rotating porous layer of viscoelastic fluid which...
Magnetohydrodynamic convection (MHD convection) in a horizontal porous-layer filled by a plasma, imb...