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|K. Thirumurugan 1, R. Vasanthakumari 2
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|Walters‟B′ fluid, Compressibility, Brinkman porous medium, Dusty particles, viscoelasticity.|
|In recent years, considerable interest has been evinced in the study of thermal instability in a porous medium because it has various applications in geophysics, food processing and nuclear reactor Rana. A detailed account of the thermal instability of a Newtonian fluid under varying assumptions of hydrodynamics and hydromagnetics has been given by Chandrasekhar . Lapwood has studied the connective flow in porous medium using linearized stability theory. The Rayleigh instability of a thermal boundary layer in flow through a porous medium has been considered by Wooding. Scanlon and Segel have considered the effect of suspended particles on the onset of Be „nard and found that the critical Rayleigh number was reduced solely because the heat capacity of pure gas was supplemented by the particles. Sharma and Sunil  have studied the thermal instability of an Oldroydian viscoelastic fluid with suspended particles in hydromagnetics in a porous medium. There are many elastico – viscous fluids that cannot be characterized by Maxwell‟s constitutive relations or Oldroyd‟s constitutive relations. One such class of elastic – viscous fluid in Rivlin – Erickson fluid. Rivlin and Erickson  have proposed a theoretical model for such another elastico – viscous fluid.|
|The investigation in porous media has been started with the simple Darcy model and gradually was extended to Darcy – Brinkman model. A good account of convection problem in a porous medium is given by vafai and Hadim , Ingham and pop  and Nield and Bejan . Kuzentsov and Nield  have studied the thermal instability of porous medium. Sharma et al. have studied the instability of streaming Rivlin-Erickson fluids in porous medium. Recently, Rana and Thakur studied the instability of couple – stress fluid permeated with suspended particles saturating a porous medium. Rana et al have studied an effect of rotation on thermal instability of compressible Walters‟B′ elastico – viscous fluid in porous medium. Shivakumara et al has studied an effect of thermal modulation on the onset of thermal convection in Walters‟B′ viscoelastic fluid in a porous medium. The interest of investigations of non – Newtonian fluids is also motivated by a wide range of engineering application which includes ground pollutions by chemicals which were non – Newtonian like lubricants and polymers in the treatment of sewage sludge in drying beds. Recently, polymers are used in agriculture, communications applications and in bio medical applications. Examples of these application filtration processes, packed bed reactors, insulation system, ceramic processing, enhanced oil recovery, chromatography etc.|
|Keeping mind the importance in various applications mentioned above, the objective of the present paper is to study the effect of suspended particles on thermal convection in Walters‟B′ elastico – viscous fluid in a brinkman porous medium. This necessitates of additional parameter namely Darcy number.|
II. MATHEMATICAL MODEL AND PERTURBATION EQUATIONS
|Consider an infinite, horizontal, compressible Walters‟ B′ elastic – viscous fluid layer fluid layer of thickness d, heated and soluted from below so that the temperatures and densities at the bottom surface z = 0 are T0 and ρ0 and at the upper surface z = 0 are Td and ρd, respectively, and that a uniform temperature gradient β(= |dT/dz|) is maintained. The gravity field g(0,0,-g), and a uniform vertical magnetic field H(0,0,H), act on the system.|
|The presence of particles adds an extra force term proportional to the velocity difference between particles and fluid and appears in the equation of motion(Eq.(1)). Since the force exerted by the fluid on the particles is equal and opposite to that exerted by the particles on the fluid, there must be an extra force term, equal in magnitude but opposite sign, in the equation of the motion for the particles (Eq.(6)). The buoyancy force on the particle is neglected. Inter particles reactions are not considered either since the distance between the particles is quite large compared with their diameters. These assumptions have been used in writing the equation of motion (Eq.(6)) for the particles. The initial state of the system is taken to be quiescent layer(no settling) with a uniform particle distribution number. The initial state is defined as Eq.(7).|
III. THE DISPERSION RELATION
|Following the normal mode analyses, we assume that the perturbation quantities have x and y and t dependence of the form|
|The dispersion relation in Eq. (30) is analysed numerically to depict the stability characteristics. In Fig. (1), Rayleigh Number 1 is plotted against suspended particles B for P = 2 and 1 = 10 for fixed wave numbers = 0.2, = 0.5. This shows that suspended particles has destabilizing effect on thermal instability of Walters‟B′ fluid in the Brinkman porous medium for fixed wave numbers = 0.2, = 0.5. Which clearly verifies the result numerically as derived in Eq. (31). In Fig. (2), Rayleigh Number R1 is plotted against with Darcy Number has a stabilizing effect on thermal convection in Walters‟B′ elastico viscous fluid permeated with dusty particles in a Brinkman porous medium which is clearly verifies the result numerically as derived in Equation (32). In Fig (3) Rayleigh number R1 is plotted against medium permeability P for 1 = 10 and B = 3 for fixed wave numbers = 0.2, = 0.5 . This slows that medium permeability has a destabilizing effect on the thermal convection in Walters‟B′ elastico-viscous fluid permeated with suspended particles in a Brinkman porous medium which is clearly verifies the result numerically as derived in Eq. (33).|
|The effect of suspended particles on thermal convection in Walters‟B′ elastico-viscous fluid heated from below in the Brinkman porous medium has been investigated. The dispersion relation, including the effects of dusty particles, Darcy number, medium permeability and viscoelasticity on the thermal convection in Walters‟B′ fluid in porous medium is derived. From the analysis, the main conclusions are as follows:|
|(iii) The effects of dusty particles, Darcy Number and medium permeability on thermal convection in Walters‟B′ elastico – viscous fluid permeated with dusty particles, in a Brinkman porous medium have been shown analyzed.|
|(iv) The oscillatory modes introduced due to the presence of viscoelasticity, dusty particles, gravity field and medium permeability, which were non – existent in their absence.|
| Chandrasekhar, S. “Hydrodynamics and Hydromagnetics stability”. New York : Dover publication, 1981.
 Ingham, D.D. and Pop L. “Transport phenomena in porous media”. New York: Elseiver, 1981.
 Kuzentsov, A.V and Nield, D.A. “Thermal instability in a porous medium layer saturated by a nano fluid. Brinkman model. Transport in Porous Media”, 81(3): 409-422. . 2010
 Lapwood, E.R. “Convection of a fluid in porous medium. Mathematical Proceedings of the Cambridge Philosophical Society”, 44:508-519. 1948
 Nield, D.A. and Bejan, A. Convection in Porous medium”. New York: Springer 2006.
 Rana G.C, “Effect of suspended particles on thermal instability of Walters‟ (model B′) fluid in a Brinckman porous medium”, IJMA, 3, 399 – 406, 2012.
 Rana G. C, Kango S.K, “Effect of rotation on thermal instability of compressible Walters‟ (model B′) elastico – viscousfluid in porous medium”, JARAM, 3, 44 – 57, 2011.
 Rana, G.C and Thakur, R.C. “A mathematical theorem on the onset of couple stress fluid permeated with suspended particles saturating a porous medium. International journal of Multiphysics” 2012.
 Rivlin R.S and ericksen, J.L.. “Stress-deformation relation for isotropic materials”. Chemistry Biodiversity, 4(2):323 – 425, 1955.
 Scanlon, J.W. and Segel, L.A. “Effect of suspended particles on the onset of Be‟nard convection”. Physics fluids,16: 1537 -1578, 1973.
 Sharma, R.C. and Sunil. “Thermal instability of an Oldroydian fluid with suspended particles in hydromagnetics in porous medium”. Polymerplastics Technology and Engineering, 33(3): 323 – 339, 1994.
 Sharma, V., Kishore, K. and Rana, G.C. “The instability of streaming Rivlin – Erickson fluids in porous medium. Studia Geotechinica et Mechanica”, 13: 83 – 93, 2001.
 Shivakumara. I.S, Lee. J, Malarshetty.M.S, Sureshkumara.S,” Effect of thermal modulation on the onset of thermal convection in Walters‟B′
viscoelastic fluid in a porous medium, transport in porous media”, 87, 297 – 307, 2011.
 Vafai, K. and Hadim, H.A. “Handbook of porous media”. New York: M.Decker, 2000.
 Wooding, R.A.. “Rayleigh instability of thermal boundary layer in flow through a porous medium. Journal of fluid mechanics”, 9:183 – 192, 1960.