On the Effect of Non-Uniform Magnetic field on the Jeans Instability of a Viscoelastic Medium

 

Joginder Singh Dhiman and Rajni Sharma

Department of Mathematics, Himachal Pradesh University, Summerhill, Shimla-171005, India.

*Corresponding Author E-mail: jsdhiman@hpuniv.ac.in; rajni22_sharma@yahoo.com

 

ABSTRACT:

In the present paper the problem of Jeans instability of a self gravitating viscoelastic medium in the presence of non-uniform magnetic field for both longitudinal and transverse mode of wave propagation under the kinetic and hydrodynamic limits has been investigated, using the generalized hydrodynamic model. It is found that magnetic field has no effect on the Jeans criterion for the onset of gravitational instability in case of longitudinal mode of wave propagation, whereas it modifies the Jeans criterion in the case of transverse mode of wave propagation and has stabilizing effect on the onset of instability. Further, it is observed that the magnetic field has no effect on the growth rate of Jeans instability of a viscoelastic medium. The effects of shear viscosity, bulk viscosity and Mach number on the Jeans criterion and on the growth rate of Jeans instability have also been studied numerically and the obtained results are depicted graphically, for both strongly coupled plasma (SCP) and weakly coupled plasma (WCP).

 

KEYWORDS: Jeans instability; viscoelastic medium; non-uniform magnetic field; wave propagation; coupled plasma.

 

1.      INTRODUCTION:

During last century, the problem of self gravitational instability has been a broad area of research in astrophysics, plasma physics and many other crucial phenomenon of the interstellar medium (Dangarh et al [1]). Jeans [2] in 1902 studied the gravitational instability of homogeneous gaseous medium and derived a criterion for the onset of instability, now known as Jeans criterion. This criterion states that the medium becomes unstable and breaks up for perturbations of the wave number  less than Jeans wave number. Here, is the density, the velocity of the sound and  is the gravitational constant. Since then several researchers have studied the problem of gravitational instability of different medium such as viscoelastic medium, plasma, anisotropic plasma, ionized plasma and dusty plasma. Rosenberg and Shukla [3] studied the instabilities in strongly coupled ultracold neutral plasmas and reported that in the field of cosmic physics strongly coupled plasmas (SCP) is of considerable interest because of possible applications to various astronomical objects like white dwarf matter, interior of heavy planets, atmosphere of neutron star and ultra cold neutral plasma. These objects are supposed to be composed of viscoelastic fluid which is strongly coupled and show both viscous and elastic behaviour. They observed that the strongly coupled state depends upon the Coulomb coupling parameter(Г), which characterizes the ratio of the electrostatic Coulomb interaction between neighboring plasma particles to the thermal (kinetic) energy of the plasma particles.When the coupling parameter Г then plasma behaves as strongly coupled plasma (SCP), when Г then plasma behaves as weakly coupled plasma (WCP). Kaw and Sen [4], Janeki et al [5] and Prajapati and Chhajlani [6] studied the gravitational instability in the viscoelastic medium, using the Generalized Hydrodynamic model (GH).The GH model describes the effects of strong correlations through the introduction of viscoelastic coefficients. Further, the GH model is valid for both the SCP as well as weakly coupled plasma (WCP).  

 

Larson [7] observed that the theoretical studies have shown that the magnetic field plays a vital role in self- gravitating star forming regions and in the evolution of interstellar clouds into self-gravitating star forming regions.  In astrophysics the problems that are considered generally assume magnetic field/rotation to be uniform. This idealization of the uniform character in theoretical investigations is valid only for laboratory purposes; however in the interstellar interior and atmosphere, the magnetic field/rotation may be variable and may alter the nature of the instability. Chandrasekhar [8] examined the individual/simultaneous effects of uniform magnetic field and rotation on the gravitational instability of the homogeneous medium and found that Jeans criterion remains unaffected. Bhatia [9] also studied the gravitational instability of plasma in the presence of a uniform rotation and uniform magnetic field and showed these have no effect on that Jeans criterion. Bel and Schatzman [10] investigated the effect of non-uniform rotation on the gravitational instability of a gaseous medium and found that the Jeans criterion gets modified due to the presence of non-uniform rotation. Further, Dhiman and Dadwal [11, 12] studied the effect of non-uniform magnetic field on the problem of gravitational instability considered by Bel and Schatzman [10] and discussed the fate of Jeans criterion under these simultaneous effects. Dhiman and Dadwal [13] studied the gravitational instability of a stratified heat conducting medium in the presence of non-uniform rotation and magnetic field and found that magnetic field, whether uniform or non-uniform, have no effects on the Jeans criterion.

 

The present paper is primarily motivated by the works of Janeki et al [5], Prajapati and Chhajlani [6], Dhiman and Dadwal [13] and the desire to investigate the effect of non-uniform magnetic field on the onset of Jeans instability in viscoelastic medium. Both longitudinal and transverse modes of wave propagation have been considered and Jeans criterion is investigated under the effect of both kinetic and hydrodynamic limits. The effects of various parameters of the problem on the growth rate of Jeans instability have also been investigated numerically and the results obtained are depicted graphically.  

 

2.      Mathematical Model and Basic Equations

Consider an infinite homogeneous, self gravitating viscoelastic fluid with infinite electrical conductivity. The system is permeated with the action of non- uniform magnetic field . Let  respectively denote the components of the velocity and magnetic field intensity in the x, y and z directions, in a rectangular co- ordinate system. Generalized hydrodynamic (GH) model has been used to treat the viscoelastic properties of the medium. The general basic equations of continuity, motions, magnetic induction and Poisson equation governing the above physical problem are given by (cf. Chapter V and Chapter XIII of Chandrasekhar [8], Janeki et al [5] and Dhiman and Dadwal [13])

 


Figure 3. The normalized growth rate of instability Re (+) to normalized wave number in the SCP and WCP for transverse mode of propagation

Figure 4. Effect of shear viscosity () on the growth rate of Jeans instability

.                                               


 

To study the effect of shear viscosity on the growth rate of Jeans instability, the values of normalized growth rate with respect to the normalized wave number  for different values of  have been calculated from equation (48) and the obtained results are depicted graphically in Figure 4. It is also observed while calculating the values of the growth rate, the real positive values of  occur only for the wave numbers  

 

3.      RESULTS AND CONCLUSIONS:

In the present paper, we have studied the self gravitating Jeans instability of a viscoelastic medium in the presence of non-uniform magnetic field, using the generalized hydrodynamic (GH) model. A general dispersion relation has been derived and cases of both the longitudinal and transverse modes of wave propagation in strongly coupled plasma (SCP) and weakly coupled plasma (WCP) under the kinetic and hydrodynamic limits have been discussed. The effect of non- uniform magnetic field on the Jeans criterion as well as on the growth rate of Jeans instability has been studied. It is observed that non-uniform magnetic field has no effect on the Jeans criterion in the longitudinal mode of propagation under the kinetic and hydrodynamic limits, whereas in the transverse mode the non-uniform magnetic field modifies the Jeans criterion under both the kinetic and hydrodynamic limits respectively. It is also observed that the non-uniform magnetic field has no effect on the growth rate of Jeans instability on both the longitudinal and transverse mode of propagation. Further, the shear viscosity and the bulk viscosity also modify the Jeans criterion for each longitudinal and transverse mode of wave propagation under the kinetic limit only. The effects of various parameters have been depicted graphically on the onset of Jeans instability under the kinetic and hydrodynamic limits. From Figure 1, it is observed that as the value of Mach number increases the instability region decreases hence has the stabilizing effect on the growth rate of Jeans instability. From Figure 2, it is observed that the growth rate of Jeans instability is larger in SCP than the WCP in the longitudinal mode. Also, from the curves in Figure 3, it is clear that growth rate is larger in WCP than in the SCP in the transverse mode of propagation. Further, Figure 4, we observe that shear viscosity has stabilizing effect on the growth rate.

 

8. REFERENCES:

1.      Dangarh B.k, Pensia, R.K,Shrivastava,V. Prajapat, V, (2011), Adv. Studies Theor. Phys., 5, 755.

2.      Jeans, J. H., (1929), Astronomy and Cosmogony, Cambridge Univ. Press.

3.      Rosenberg, M. and Shukla, P.K., (2011), Phys. Scr. 83, 015503

4.      Kaw, P.K. and Sen, A., (1998), Phys. Plasmas 5, 3552. Larson, R. B., (2003),Rep. Prog. Phy, 66, 1651.

5.      Janaki, M.S., Chakrabarti, N. and Benerjee, D., (2011),J, Phys. Plasmas 18, 012901.

6.      Prajapati, R. P. and Chhajlani, R. k., (2013), Astrophys. Space Sci. 344, 371.

7.      Larson, R. B., (2003),Rep. Prog. Phy, 66, 1651.

8.      Chandrasekhar, S., (1961), “Hydrodynamics and Hydromagnetic Stability”. Oxford Clarendon.

9.      Bhatia P.K, (1969) Nuovo Cimento. 59, 228–235.  

10.    Bel, N. and Schatzman, E., (1958), Rev. Mod. Phys., 30, 1015.

11.    Dhiman, J. S., and Dadwal, R., (2010), Astrophys. Space Sci., 325(2), 195.

12.    Dhiman, J. S., and Dadwal, R., (2011), Astrophys. Space Sci., 332, 373.

13.    Dhiman, J. S., and Dadwal, R., (2012), J. Astrophys.Astr.33, 363. 

 

 

Received on 04.01.2014                    Accepted on 02.02.2014

© EnggResearch.net All Right Reserved

Int. J. Tech. 4(1): Jan.-June. 2014; Page 07-12