Author(s):
Anu Sharma, Neeti Goel
Email(s):
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Anu Sharma1, Neeti Goel2
1 Department of Mathematics, Rajdhani College, University of Delhi, Raja Garden,
Ring Road, New Delhi, 110015, India.
2Department of Mathematics, Acharya Narendra Dev College, University of Delhi,
Govindpuri, Kalka Ji, New Delhi, 110019, India.
*Corresponding Author
Published In:
Conference Proceeding, Mathematics in Space and Applied Sciences (ICMSAS-2023)
Year of Publication:
March, 2023
Online since:
March 04, 2023
DOI:
Study of lack of thermal equilibrium and anisotropy
effects on double-diffusive ferroconvection in porous medium
Anu Sharma1, Neeti Goel2
1 Department of Mathematics, Rajdhani College, University of Delhi, Raja
Garden,
Ring Road, New Delhi, 110015, India.
2Department of Mathematics, Acharya Narendra Dev College, University of
Delhi,
Govindpuri, Kalka Ji, New Delhi, 110019, India.
*Corresponding
Author E-mail:
ABSTRACT:
In this work, we study
theoretically the effect of lack of local thermal equilibrium and anisotropy on
double-diffusive ferro convection in aporous medium. Stability analysis is
carried out for ferrofluid layer contained between two stress-free boundaries
using normal mode method. The eigen value problem is solved using regular
perturbation technique to obtain critical thermal Rayleigh number. The impact
of anisotropy parameter of permeability of porous medium, heat transfer
coefficient and salinity Rayleigh number on the onset of convection are
examined.
KEYWORDS: Ferrofluid, Double-diffusive convection, Anisotropic
porous medium, Local thermal equilibrium.
1.
INTRODUCTION
In
double-diffusive convection problems, there are two destabilizing sources for
density difference, the temperature field and salt field. Double diffusion was
first explored because of its application to oceanic phenomenon. When a fluid
permeates through a porous material the flow is analyzed by macroscopic law,
called Darcy law as referred byLapwood [1].In literature majority of the studies on convection in porous mediumhave
been dealt with local thermal equilibrium conditions. In many situations (Nield
andBejan[2]), lackof local thermal equilibrium exists. In such cases local
thermal nonequilibrium effects are to be considered by two field model energy
equationrepresenting fluid and solid phases separately. An excellent review of
research on local thermal non-equilibrium phenomenon in porous medium
convection, primarily free and forced convection boundary layers and free
convection within cavities is given by Rees and Pop [3].
Ferrofluids are
electrically non-conducting colloidal suspensions of tiny magnetic particles
coated with surfactant
immersed in a carrier fluid. These fluids behave as continuum and
exhibit a variety of
interesting phenomenon. Ferrofluids are widely used in magnetic inkjet
printers, inertial dampers,
switches, sensors, magnetic and nanofluidic devices, magnetic targeted drug
delivery etc. Rosenweig[4] reviews several applications of heat transfer
through ferrofluids. This heat transfer through ferrofluids is called ferroconvection.
The study of convection in two component ferrofluids is referred as
double-diffusive ferroconvection studied by Baines and Gill [5] and later on
extensively studied by many authors [6-9].
Most of the studies have
been concerned with isotropic media, but geological and pedagogical processes
rarely form isotropic porous media.Vaidyanathan et al. [10] studied
ferroconvection in an anisotropic densely packed porous medium.Suresh et al. [11]
studied numerical analysis of ferroconvection with temperature dependent
viscosity and anisotropic porous medium. In the present work, it is attempted
to analyze the effect of lack of thermal equilibrium and anisotropy effect on
double-diffusive convection in ferrofluid layer saturated porous medium and free
boundaries are considered. An analytical formula is found for critical Rayleigh
number to study effect of various parameters.
2 MATHEMATICAL
FORMULATION
An infinite
incompressible ferrofluid saturated an anisotropic porous layer of thickness ‘
’ heated from below and soluted from below in the presence of
uniform vertical magnetic field is considered. A constant temperature gradient
and solute gradient is maintened across the layer. Darcy model for flow through
porous medium with fluid and solid phases not in thermal equilibrium is
considered. With these assumptions the basic goverening equations are
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