Conference Proceeding

Mathematics in Space and Applied Sciences (ICMSAS-2023)
ICMSAS-2023

Subject Area: Mathematics
Pages: 331
Published On: 03-Mar-2023
Online Since: 04-Mar-2023

 Read More >>

Author(s): Chitresh Kumari, Jitender Kumar, Harjinder Singh, Jyoti Prakash

Email(s): chitreshsharma9098@gmail.com

Address: Chitresh Kumari*, Jitender Kumar, Harjinder Singh, Jyoti Prakash
Department of Mathematics & Statistics, Himachal Pradesh University, Shimla-171005.
*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:




On exchange Principle in Multicomponent Convection with Viscosity Variations

 

Chitresh Kumari*, Jitender Kumar, Harjinder Singh, Jyoti Prakash

Department of Mathematics & Statistics, Himachal Pradesh University, Shimla-171005.

*Corresponding Author E-mail: chitreshsharma9098@gmail.com

 

Abstract:

In the present paper, the multicomponent convection problem has been studied by considering variable viscosity. A sufficient condition has been derived for the validity of the occurrence of stationary convection. Further the results derived herein are uniformly valid for all combinations of the bounding surfaces.

 

Keywords: Multicomponent Convection, Stationary Convection, Principle of the Exchange of Stabilities, Variable Viscosity.

 

INTRODUCTION:

In many fluid systems, density depends on more than three independently stratifying agencies having different diffusivities which is known as multicomponent diffusive convection. It is an interesting topic for the researchers due to its manifold applications. Examples of multicomponent diffusive convection fluids includes magmas and their laboratory models, earth’s core and sea water (Griffiths et. al. (1979) and Terrones (1993)), solidification of molten alloys and exothermally heated lakes.

 

Several researchers have shown their interest in this field of enquiry. Griffiths (1979) and Pearlstein et al.(1989) studied the onset of convection in a horizontally infinite layer of a triply diffusive fluid. The general case of n independently diffusing stratifying agencies has been considered by Terrones and Pearlstein (1989). Ryzhkov and Shevtsova (2007) investigated the case of multicomponent mixture with application to the thermogravitational column. Ryzhkov and Shevtsova (2009) also investigated the longwave instability of a multicomponent fluid layer with Soret effect. Rionero (2013) examined the multicomponent diffusive-convective fluid motions in porous layer. For a broad view of the subject one may also be referred to Turner (1985), Tracey (1996), Straughan and Tracey (1999).

 

Since the effect of viscosity variation plays an important role in several physical situations. Therefore, it is necessary to extend the classical analysis wherein the fluid viscosity is a function of temperature and/or depth (Banerjee et.al.(1977), Prakash et al.(2015)). Further, the change of viscosity with temperature is extremely rapid, the inclusion of variation effects certainly extends the domain of validity of the existing results in the literature. From a mathematical point of view, the resulting differential equations have variable coefficients contrary to the case wherein viscosity is constant and therefore these more general problems introduce extra analytical complexities. In the present paper, we make an attempt to mathematically handle these more complex problems in the case of multicomponent convection.

 

The “principle of the exchange of stabilities”, which implies that convection occurs initially as stationary convection or we can say that all non-decaying disturbances are non-oscillatory in time which further implies that the first unstable eigen value of the linearized system has imaginary part equal to zero (Herron (2000)) due to which mathematical handling of the governing equations becomes easy. Therefore, the aim of the present paper is to establish a sufficient condition for the validity of “principle of the exchange of stabilities” in multicomponent convection problem with variable viscosity.

 

The Physical Problem:

The physical problem consists of an infinite horizontal layer of a Boussinesq viscous fluid which is statically confined between two horizontal boundaries  and  maintained at constant temperatures  and  and uniform solute concentrations   and  … … …  at the lower and upper boundaries respectively.




REFERENCES:

1.              Banerjee, M.B., Gupta, J.R. and Shandil, R.G. (1977): Generalized thermal convection with viscosity variations, J. Math.Anal. Appl. 167(1), 66-73.

2.              Chandrasekhar, S. (1981): “Hydrodynamic and Hydromagnetic Stability”, Oxford university Press, dover publication, Inc., New York.

3.              Griffiths, R.W. (1979): The influence of a third diffusive component upon the onset of convection, journal of fluid mechanics, 92, 659-670.

4.              Gupta, J.R., Sood, S.K. and Bhardwaj, U.D. (1986): On the characterization of non-oscillatory motions in a rotatory hydromagnetic thermohaline convection, Ind. J. Pure appl. Math., 17(1), 100-107.

5.              Herron, I., (2000): On the principle of exchange of stabilities in Rayleigh-Benard convection, SIAM J. Appl. Math., 61(4), 1362-1368.

6.              Pearlstein, A. J., Harris, R.M., Terrones, G. (1989): The onset of convective instability in a triply diffusive fluid layer, J. Fluid Mech., 202, 443-465.

7.              Prakash. J., Kumar, R., Kumari, K., (2015a): A characterization theorem in triply diffusive convection with viscosity variations, Raj. Acad. Phys. Sci., 14 (3&4),249-258.

8.              Prakash. J., Kumar, R., Kumari, K., (2015b): Linear triply diffusive convection with viscosity variations, Int. J. Phys. and Math. Sciences, 5(1), 186-196.

9.              Prakash.J and Manan, S. (2016): On rotatory hydromagnetic multicomponent convection, Int. J. Appl. Sci. Eng. Res., 5(6), 405-420.

10.           Rionero, S. (2010): Long time behaviour of multicomponent fluid mixtures in porous media, Int. J. Eng. Sc.,48, 1519-1533.

11.           Rionero, S. (2013): Multicomponent diffusive-convective fluid motions in porous layers: Ultimately boundedness, absence of subcritical instabilities, global non-linear stability for any number of salts, Phys. Fluids, 25, 054104(1-23).

12.           Ryzhkov, I.I. and Shevtsova, V.M. (2007): On thermal diffusion and convection in multicomponent mixtures with application to the thermogravitational column. Phys. Fluids, 19(2), 027101(1-17).

13.           Ryzhkov, I.I. and Shevtsova, V.M. (2009): Long wave instability of a multicomponent fluid layer with the soret effect. Phys. Fluids, 21(1), 014102(1-14).

14.           Schultz, M.H. (1973): “Spine Analysis”, Prentice-Hall Englewood cliffs NJ.

15.           Stengel, K.C., Oliver, D.S. and Booker, J.R. (1982): Onset of convection in variable viscosity fluid, J. Fluid Mech., 120, 411-431.

16.           Terrones, G. (1993): Cross-diffusion effects on the stability criteria in a triply diffusive system, Phys, Fluids A, 5, 2172-2182.

17.           Terrones, G., and Pearlstein, A.J., (1989): The onset of a convection in a multicomponent fluid layer, Phys, Fluids A, 1(5), 845-853.

18.           Tracey, J. (1996): Multi-component convection-diffusion in a porous medium, Contum. Mech. Thermodyn., 8(6), 361-381.

19.           Turner, J.S., (1985): Multicomponent convection, Annu. Rev. Fluid Mech., 17, 11-44.

 

 

 



Related Images:



Author/Editor Information

Dr. Sanjay Kango

Department of Mathematics, Neta Ji Subhash Chander Bose Memorial, Government Post Graduate College, Hamirpur Himachal Pradesh-177 005, INDIA