Heat Transport in an Anisotropic Porous Medium Saturated with Variable Viscosity Liquid Under G-jitter and Internal Heating Effects
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Abstract
Thermo-rheological effect of temperature-dependent viscous fluid saturating a porous medium has been studied in the presence of imposed time periodic gravity field and internal heat source. Weak nonlinear stability analysis has been performed by using the power series expansion in terms of the amplitude of gravity modulation, which is considered to be small. Nusselt number is calculated numerically using Ginzburg–Landau equation. The nonlinear effects of thermo-mechanical anisotropies, internal heat source parameter, Vadász number, thermo-rheological parameter and amplitude of gravity modulation have been obtained and depicted graphically. Streamlines and isotherms have been drawn for different times. Comparisons have been made between various physical systems.
Keywords
Ginzburg–Landau model Gravity modulation Porous media Anisotropy Temperature-dependent viscosity Internal heat source Nonlinear stabilityList of Symbols
Latin Symbols
- \(A\)
Amplitude of convection
- \(a_1\)
Amplitude of gravity modulation
- \(d\)
Depth of the fluid layer
- \(\mathbf g \)
Acceleration due to gravity
- \(k_{\mathrm{c}}\)
Critical wave number
- \(K_{x}\)
Permeability in x-direction
- \(K_{z}\)
Permeability in z-direction
- \(Nu\)
Nusselt number
- \(p\)
Reduced pressure
- \(R_{\mathrm{i}}\)
Internal heat source parameter \(R_{\mathrm{i}}=\frac{Q d^2}{\kappa _{Tz}}\)
- \(Ra_{\mathrm{T}}\)
Thermal Rayleigh number, \(Ra_{\mathrm{T}}=\frac{\beta _{\mathrm{T}} g _0 \Delta T d K_{z}}{\nu \kappa _{Tz}}\)
- \(R_{\mathrm{0c}}\)
Critical Rayleigh number
- \(T\)
Temperature
- \({Va}\)
Vadász number \({Va}=\frac{\nu d^2}{K_z\kappa _{Tz}}\)
- \(V\)
Thermo-rheological parameter \(V=\delta _0 {\Delta T} \)
- \(\Delta T\)
Temperature difference across the porous layer
- \(t\)
Time
- \((x,z)\)
horizontal and vertical coordinates
Greek Symbols
- \(\beta _{\mathrm{T}}\)
Coefficient of thermal expansion
- \(\delta _0\)
Small parameter indicating variation of viscosity with temperature
- \(\delta ^2\)
Horizontal wave number \(\delta ^2=k_{\mathrm{c}}^2+\pi ^2\)
- \(\epsilon \)
Perturbation parameter
- \(\gamma \)
Heat capacity ratio \(\gamma =\frac{(\rho c)_{\mathrm{m}}}{(\rho c)_{\mathrm{f}}}\)
- \(\eta \)
Thermal anisotropy parameter \(\kappa _{Tx} /\kappa _{Tz}\)
- \(\xi \)
Mechanical anisotropy parameter \( K_{x} /K_{z}\)
- \(\varOmega \)
Frequency of modulation
- \(\kappa _{T}\)
\(\kappa _{Tx} (ii + jj) + \kappa _{Tz} (kk)\)
- \(\kappa _{Tx}\)
Effective thermal diffusivity in \(x\)-direction
- \(\kappa _{Tz}\)
Effective thermal diffusivity in \(z\)-direction
- \(\mu \)
Dynamic viscosity of the fluid
- \(\phi \)
Porosity
- \(\nu \)
Kinematic viscosity, \(\left( {\frac{\mu }{\rho _{0}}} \right) \)
- \(\rho \)
Fluid density
- \(\psi \)
Stream function
- \(\tau \)
Slow time \(\tau =\epsilon ^2 t\)
- \(\varTheta \)
Perturbed temperature
Other Symbols
- \(\nabla _{1}^2\)
\(\frac{\partial ^{2}}{\partial x^{2}}+\frac{\partial ^{2}}{\partial y^{2}}\)
- \(\nabla ^{2}\)
\(\nabla _{1}^2+\frac{\partial ^{2}}{\partial z^{2}}\)
Subscripts
- b
Basic state
- c
Critical
- 0
Reference value
Superscripts
- \(^{\prime }\)
Perturbed quantity
- \(*\)
Dimensionless quantity
- st
Stationary
Notes
Acknowledgments
This work was done during the lien sanctioned to the author by Banaras Hindu University, Varanasi to work as professor of Mathematics at Department of Applied Mathematics, School for Physical Sciences, BB Ambedkar University, Lucknow, India. The author BSB gratefully acknowledges Banaras Hindu University, Varanasi for the same. Further, author Alok Srivastava gratefully acknowledges the financial assistance from Banaras Hindu University as a research fellowship.
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