Thermal Instability of Ferromagnetic Fluid in the Presence of Hall Effect and Suspended Particle under Varying Gravity Field

 

S. K. Kango1, Vikram Singh2 and Virender Singh3

1Department   of   Mathematics, Govt. College, Haripur (Manali)  (H,P.) – 175136 (INDIA)

2Department of Mathematics, Jwalaji Degree College, Jwalamukhi (H,P.) – 176031 (INDIA)

3Department of Mathematics, Jwalaji Degree College, Jwalamukhi (H,P.) – 176031 (INDIA)

*Corresponding Author E-mail: skkango72@gmail.com; vsmanhas23@gmail.com; virenderbharoli@gmail.com

 

ABSTRACT:

In this paper we consider theoretical investigation of the effect hall current and  the suspended particle under varying gravity field on the thermal instability of ferromagnetic  fluid heated from below. For a fluid layer between two free boundaries and exact  solution is obtained using a linearized stability theory and normal mode analysis . A dispersion relation governing the effect of  hall current and  the suspended particle is obtained. For the case of stationary convection it is found that the magnetic field has a stabilizing  the system when the gravity is increasing upward  i.e. (), where as the hall current and suspended particle are found to have the destabilizing  effect on the system when the gravity is increasing upward  i.e. (). The critical Rayleigh numbers and wave numbers of the associated disturbances for the onset of stability as stationary convection are obtained. The principle of exchange of stabilities is not valid for the problem under consideration, whereas in the absence of Hall currents

hence magnetic field, it is valid under certain conditions.

 

KEYWORDS: Hall currents, suspended particles, ferromagnetic fluid and  varying  gravity field.

 

1.      INTRODUCTION:

 Ferrohydrodynamics deals with the mechanics of fluid motions influenced with the mechanics of fluid motions influenced by strong forces of magnetic polarization.  The Ferrohydrodynamics concerns usually with the interaction of magnetic field on  conducting as well as non-conducting ferromagnetic fluids. The polarization force and the body  couple are the two main features that distinguish a ferromagnetic fluid from an ordinary fluid. Ferromagnetic fluids are electrically non conducting colloidal suspensions of solid ferromagnetic  particles in a

non –electrically  conducting carrier fluid like water, kerosene, hydrocarbon etc. A Ferromagnetic fluid contains 1023 particles per cubic meter. These fluids behave as a homogeneous continuum and exhibit a variety of interesting phenomena. Ferromagnetic fluids are not found in nature but are artificially synthesized.           

 

A detailed introduction to this fascinating subject has been given in the celebrated monograph by Rosensweig (1985). This monograph reviews several applications of heat transfer through magnetic fluids. One such phenomenon is enhanced convicted cooling having a temperature dependent magnetic moment due to magnetization of the fluid. This magnetization, in general, is a function of the magnetic field, temperature and density of the fluid. A variation of any of these causes a change of body force. This leads to convection in Ferromagnetic fluids in the presence of the magnetic field gradient. This mechanism is known as ferro convection, which is similar to Benard convection (Chandrasekhar, 1981). In our analysis, we assume that magnetization is aligned with the magnetic field. Convective stability of a Ferromagnetic fluid for a fluid layer heated from below in the presence of uniform vertical magnetic field was considered by Finlayson (1970). He explained the concept of thermo-mechanical interaction in Ferromagnetic fluids.  Thermoconvetive stability of a Ferromagnetic fluid without considering buoyancy effect was investigated by Lalas and Carmi (1971) whereas Shliomis (1974) analyzed the linealized relation for magnetized perturbed quantities at the limit of stability. In geophysical situation, the fluid is often not pure but contains suspended particles. Scanlon and Segel (1973) investigated some of the continuum effects of particles on Benard convection and found that a critical Rayleigh number was reduced solely because the heat capacity of the pure was supplemented by that of the particles. The effect of the suspended particles was thus found to destabilized the layer. The effect of the suspended particles on non magnetic fluids has been investigated by many authors (Sharma et al., 1976; Sharma and Aggarwal, 2006). The main results from these studies are that suspended particles have a destabilizing effect on the system and the fact that the specific heat of a fluid is greater than the specific heat of the particles is the sufficient condition for the non-existence of over stability. The effect of suspended particles and rotation o thermal stability of Ferromagnetic fluids is studied by Aggarwal and Prakash (2009) .         

In the presence of a strong electric field, electric conductivity is affected by the magnetic field. Consequently, the conductivity parallel to the electric field is reduced. Hence, the current is reduced in the direction normal to both the electric and magnetic field is known as ‘Hall effect’. The Hall current is likely to be important in many geophysical and astrophysical situations as well as in flows of laboratory plasmas. The effect of Hall current on thermal stability has also been studied by many other authors  as Raghavachar and Gothandaraman (1988), Sharma and Gupta (1993), Gupta (1967).

 

Soon after the development of the method of formation of Ferromagnetic fluids in the early or mid 1960s, the importance of Ferrohydrodynamics was realized. Due to the vide  ranges of application  of  Ferromagnetic fluids to instrumentation, lubrication, printing, vacuum technology, vibration damping, metal recovery, acoustics and medicine, their commercial usage includes vacuum feed through for semiconductor  manufacturing and related uses (Moskowitz,  1975),  pressure  seals for compressors and blowers (Roseasweig, 1979). They are also used in liquid cooled loudspeakers that involve small bulk quantities of Ferromegnetic fluids to conduct heat away from the speaker coil (Hathaway, 1979). This innovation increases the amplifying power of the coil, and hence it leads the loudspeakers to produce high fidelity sound. In order to bring drugs to a target site in a human body, a magnetic field can pilot the path of a drop of the ferromagnetic fluid in the human body (Morimoto et al., 1982). The novel zero leakage rotating shaft seal are used in computer disc drives (Bailey, 1983). Experimental and theoretical physicists and engineers contributed significantly to Ferrohydrodynamics and its applications (Odenbach, 2002). During the last half century, research on magnetic liquid has been very productive in many fields. Strong efforts have been undertaken to synthesized stable suspensions of magnetic particles with different performances in magnetism, fluid mechanics or physical chemistry.

 

Keeping in view the above mentioned significance, the present problem, therefore deals with the thermal instability of a ferromagnetic fluid heated from below in the presence of  uniform magnetic field under the influence of Hall currents and suspended particles under varying gravity field. In this problem we have extended the earlier  results by Sharma and Aggarwal (2006), Aggarwal and Makhija (2012) under varying gravity field  for a incompressible  ferromagnetic  fluid.

 

8. CONCLUSION:

In the present paper, the following observations have been derived from the study conducted the combined effect of suspended particles, magnetic field and hall currents on thermal stability of a  ferromagnetic fluid under varying gravity field has been considered. The effect of various parameters such as the magnetic field, hall currents and suspended particles have been investigated analytically. The principle conclusions are:-

                 I.          In order to investigate the effects of the magnetic field suspended particles  and Hall current, we examined the behavior of dR1/dQ, dR1/dH1  and dR1/dM analytically.

                II.          It is observed that magnetic field has stabilizes the system when the gravity is increasing upward and destabilizes the system when the gravity is decreasing upward. It is also shows that suspended particles and hall current have a stabilizing or  destabilizing effects on thermal convection as gravity decreasing or increasing upwards.

              III.          The principle of exchange of stability is not valid in the problem whereas in the absence of magnetic field it is valid under certain condition if

 

9. REFERENCES:

Chanderasekhar S. (1981): Hydrodynamic and Hydromagnetic Stability- New York; Dover Publications.

Finlayson B. A. (1970): Convective stability of ferromagnetic fluids  - J. Fluid , Mech., vol.40, pp.753-767.

Gupta A.S. (1967): Hall Effects on Thermal Stability- Rev. Roum.Maths. Pure Applied, vol 12, pp. 665-677.

Hatheaway D.B. (1979) : Use of ferromagnetic fluids in moving coil loudspeakers. – dBSoundEng. Mag., vol 13, pp.42-44.

Lalas D.P. and Carmi S.(1971): Thermoconvective  stability of  ferromagnetic fluids.- Phys. Fluids, vol.14, pp.436-437.

Moromoto Y., et. Al., (1982): Dispersion state of protein-stabilized Magnetic Emulsion.- Chem. Pharm. Bull., vol.30, pp. 3024-3027.

Rosenwieg R.E. (1985): Ferrohydrodynamics – Cambridge; Cambridge University Press.

Raghavachar M. R. and Gothandaraman V. S. (1988): Hydromagnetic Convection in a roatating fluid layer in the presence of Hall Current.-Geophys. Astro. Fluid Dyn., vol.45, pp.199-211.

Bailey R.L. (1983): lesser knoen applications of ferromagnetic fluids -  J.Magn. mater., vol.39, pp.178-182.

Aggarwal A.K. and Prakash K. (2009): Effect of suspended particles and rotation on thermal stability of ferromagnetic fluids.- Int. J. of  Applied Machanics and Engineering, vol. 14, No.1, pp.55-66.

Sharma R. C. and Gupta U. (1993): Thermal stability of Compressible Fluids with Hall Current and Suspended Particles in Porous medium.-Int. Journal of Eng. Sci., vol.31, No. 07, pp. 1053-1060.

Aggarwal A.K. and Makhija S. (2012): Hall Effect on Thermal Stability of Ferromagnetic Fluid in the Presence of Suspended Particles.- Int. J. of Applied Mechanics and Engineering, 2012, vol. 17, No. 2, pp.349-365.

 

 

Received on 14.01.2014    Accepted on 31.01.2014

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