Abstract
The effect of rotation and anisotropy on the onset of double diffusive convection in a horizontal porous layer is investigated using a linear theory and a weak nonlinear theory. The linear theory is based on the usual normal mode technique and the nonlinear theory on the truncated Fourier series analysis. Darcy model extended to include time derivative and Coriolis terms with anisotropic permeability is used to describe the flow through porous media. The effect of rotation, mechanical and thermal anisotropy parameters, and the Prandtl number on the stationary and overstable convection is discussed. It is found that the effect of mechanical anisotropy is to allow the onset of oscillatory convection instead of stationary. It is also found that the existence of overstable motions in case of rotating porous medium is not restricted to a particular range of Prandtl number as compared to the pure viscous fluid case. The finite amplitude analysis is performed to find the thermal and solute Nusselt numbers. The effect of various parameters on heat and mass transfer is also investigated.
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Abbreviations
- a :
-
Wsavenumber, \(\sqrt{l^{2}+m^{2}}\)
- d :
-
Height of the porous layer,
- Da :
-
Darcy number, K z /d 2
- g :
-
Gravitational acceleration, (0,0,-g)
- H :
-
Rate of heat transport per unit area
- J :
-
Rate of mass transport per unit area
- K :
-
Permeability tensor, K −1 x (ii + jj ) + K −1 z (kk)
- l, m :
-
Horizontal wavenumbers
- Nu :
-
Thermal Nusselt number
- Nu S :
-
Solute Nusselt number
- p :
-
Pressure
- Pr:
-
Prandtl number, ν /κ Tz
- q :
-
Velocity vector, (u, v, w)
- Ra T :
-
Thermal Rayleigh number, β T gΔTdK z ν /κ Tz
- Ra S :
-
Solute Rayleigh number, β S gΔTdK z ν /κ Tz
- R T :
-
Scaled Rayleigh number, Ra T /π 2
- R S :
-
Scaled solute Rayleigh number, Ra S /π2
- t :
-
Time
- t 1 :
-
Rescaled time, χ t
- T :
-
Temperature
- Ta :
-
Taylor number, (2ΩK z /ν)2
- S :
-
Solute concentration
- ΔT :
-
Temperature difference between the walls
- ΔS :
-
Salinity difference between the walls
- x, y, z :
-
Space coordinates
- α :
-
Scaled wavenumber, a 2/π2
- β T :
-
Thermal expansion coefficient
- β S :
-
Solute expansion coefficient
- γ :
-
Scaled Darcy–Prandtl number, χ /π 2
- ε :
-
Porosity
- κ T :
-
Thermal diffusivity tensor, κ Tx (ii + jj) + κ T_z (kk )
- κ S :
-
Solute diffusivity
- χ :
-
Darcy–Prandtl number, ε Pr/Da
- η :
-
Thermal anisotropy parameter, κ Tx /κ Tz
- τ :
-
Diffusivity ratio κ S /κ Tz
- μ :
-
Dynamic viscosity
- ν :
-
Kinematic viscosity, μ /ρ 0
- ρ :
-
Density
- σ :
-
Growth rate
- ω :
-
Vorticity vector, ∇ × q
- Ω :
-
Angular velocity, (0, 0, Ω )
- ξ :
-
Mechanical anisotropy parameter, K x /K z
- ψ :
-
Stream function
- \(\nabla_h^2\) :
-
\(\frac{\partial^{2}}{\partial x^{2}}+\frac{\partial ^{2}}{\partial y^{2}}\)
- ∇2 :
-
\(\nabla_h^2 +\frac{\partial ^{2}}{\partial z^{2}} \)
- b :
-
Basic state
- c :
-
Critical
- f :
-
Fluid
- h :
-
Horizontal
- 0 :
-
Reference
- s :
-
Solid
- *:
-
Dimensionless quantity
- / :
-
Perturbed quantity
- osc :
-
Oscillatory state
- st :
-
Stationary
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Malashetty, M.S., Heera, R. The Effect of Rotation on the Onset of Double Diffusive Convection in a Horizontal Anisotropic Porous Layer. Transp Porous Med 74, 105–127 (2008). https://doi.org/10.1007/s11242-007-9183-7
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DOI: https://doi.org/10.1007/s11242-007-9183-7