Research Article

Nonlinear Propagation of Dust-Ion-Acoustic Shock Waves in a Degenerate Multi-Species Plasma

^{1}Department of Physics, Jagannath University, Dhaka-1100, Bangladesh^{2} Department of Physics, Jahangirnagar University, Savar, Dhaka-1342, Bangladesh

***Corresponding author: Promi Halder**, Assistant Professor, Department of Physics, Jagannath University, Dhaka-1100, Bangladesh, Tel: (+880)1775167522, E-mail: promi.plasma@gmail.com

**Received:** April 30, 2019 **Accepted:** May 13, 2019 **Published:** May 20, 2019

**Citation:** Halder P, Mukta KN, Mamun AA. Nonlinear Propagation of Dust-Ion-Acoustic Shock Waves in a Degenerate Multi-Species Plasma. *Int J Cosmol Astron Astrophys*. 2019; 1(3): 81-87. doi: 10.18689/ijcaa-1000119

**Copyright:** © 2019 The Author(s). This work is licensed under a Creative Commons Attribution 4.0 International License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

The nonlinear propagation of dust-ion-acoustic (DIA) waves in an unmagnetized collisionless degenerate dense plasma (containing degenerate electron, positron, ion fluids and negatively charged dust grains) have been theoretically investigated. The Burgersʼ equation has been derived by employing the reductive perturbation method and by taking the effect of viscous force in the ion fluid into account. The stationary shock wave solution of Burgersʼ equation is obtained, and numerically analyzed in order to identify the basic properties of dust-ion-acoustic shock structures. It has been shown that depending on plasma parametric values, the degenerate plasma under consideration supports compressive or rarefactive shock structures. The relevance of our results in astrophysical objects like white dwarfs and neutron stars, which are of scientific interest, are briefly discussed.

PACS numbers: 52.27.Ny, 52.35.Fp, 52.35.Tc, 52.25.Vy

**Keywords:** Dust-ion-acoustic waves; Shock waves; Degenerate pressure; Relativistic factor; Compact objects.

Introduction

Now-a-days, the linear properties of the DIA waves in dusty plasmas are well understood from both theoretical and experimental points of view [1-5]. Recently, the nonlinear waves particularly the DIA shock waves (DIA ShWs) have received an impressive interest in realizing the basic properties of localized electrostatic perturbations in space and laboratory dusty plasmas. The physics of quantum plasmas, rapidly grown beyond conventional plasmas found in space or laboratory for many years [6,7]. This is mainly due to the potential applications of quantum plasmas in different areas of scientific and technological importance [8-11]. It is a common idea that electron-positron plasmas have presumably appeared in the early universe [12,13] and are frequently encountered in active galactic nuclei [14] and in pulsar magnetospheres [15,16]. This electron-positron-ion plasma is usually characterized as a fully ionized gas consisting of electrons and positrons of equal masses. Recently, there has been a great deal of interest in studying linear as well as nonlinear wave motions in such plasmas [17,19]. However, most of the astrophysical plasmas usually contains ions, in addition to the electrons and positrons. Clearly, the properties of wave motions in an electron-positron-ion plasma should be different from those in two-component electron-positron plasmas. For example, Rizzato [20] and Berezhiani et al. [21] have investigated envelope solutions of electromagnetic waves in three-component electron-positron-ion plasmas.

The electron-positron-ion plasmas are thought to be generated naturally by pair production in high energy processes in the vicinity of several astrophysical objects as well as produced in laboratory plasmas experiments with a finite life time [22]. Because of the long life time of the positrons, most of the astrophysical [23] and laboratory plasmas [24] become a mixture of positrons, which is the analog of recombination in plasma composed of ions and electrons, is relatively unimportant in classical [25], as well as in dense plasmas [26] to study the collective plasma oscillations. The ultra dense degenerate electron-positron plasmas with ions are believed to be found in compact astrophysical bodies like neutron stars and the inner layers of white dwarfs [26-29] as well as in intense laser-matter interaction experiments [30,31].

Now-a-days, a number of authors have become interested to study the properties of matter under extreme conditions [32-36]. Recently, a number of theoretical investigations have also been made of the nonlinear propagation of electrostatic waves in degenerate quantum plasma by a number of authors [37-39] etc. However, these investigations are based on the electron equation of state valid for the non-relativistic limit. Some investigations have been made of the nonlinear propagation of electrostatic waves in degenerate dense plasma based on the degenerate electron equation of state valid for ultra relativistic limit [40-42]. We are interested to study the dissipation relation of the DIA ShWs in a degenerate e-p-i plasma system where we have added positrons for the rather long lifetime of positrons, most of the astrophysical [14,16-18,23,29,43-45] as we have mentioned in the introductory chapter. The DIA ShWs are longitudinal oscillations of the ions (and the electron-positron) a dusty e-p-i plasma. The linear dispersion relation (DR) will give the relation between the wave frequency 'ω and the wave number 'κ. The number density of the degenerate electron and positron in a compact object is so high (e. g. in white dwarfs, the degenerate electron number density can be order of 10^{36} cm^{-3} even more, and order of 10^{36} cm^{-3} even more in neutron stars) that the non-relativistic limit is not practically applicable for de-generate fermions (electron-positron-ions). The equation of state for degenerate particles in astrophysical compact objects is the ultra-relativistic limit mathematically explained by S. Chandrasekhar [33]. It is very important to note that the degenerate pressure depends only on the fermion number density, but not on its temperature.

To the best of our knowledge, no theoretical investigation has been developed to study the extreme condition of matter for both non-relativistic and ultra-relativistic limits in a degenerate plasma system with the nonlinear propagation and formation of the dust-ion-acoustic shock waves (DIA ShWs). Therefore, in our present investigation, we consider a degenerate dense plasma system in absence of the magnetic field containing nonrelativistic degenerate cold ion fluid, both non-relativistic and ultra-relativistic degenerate electrons and positrons where the ion is the heavier element among all other elements. To study the basic features of the dust-ion-acoustic nonlinear structures of shock wave in such unmagnetized three component degenerate dense plasma, we have studied the Burgersʼ equation and the numerical solution of Burgersʼ equation. The model is relevant to compact interstellar objects (e. g., white dwarf, neutron star, etc.) [46].

**Governing equations**

We consider an unmagnetized collisionless degenerate dense plasma system consisting of non-relativistic degenerate cold degenerate ion fluid and both non-relativistic and ultra-relativistic degenerate electrons and positrons fluids and negatively charged dust grains. The dynamics of the one dimensional DIA ShWs in such a degenerate dense plasma system is governed by

where *μ* is the ratio of the number density of negatively charged dust and ion (*Z _{d}n_{d0}/n_{io}*) &

*μ*=1+

*α*is the plasma number density of the species s (s = e for electron, i for ion, and p for positron) normalized by its equilibrium value

_{p}-α_{e},n_{s}*n*, is the plasma species fluid speed normalized by

_{so}(n_{eo}), u_{s}*C*

_{im}=(m_{e}c^{2}/m_{i})^{1/2}with

*m*being the electron (ion) rest mass mass and

_{e}(m_{i})*c*being the speed of light in vacuum,

*Φ*is the electrostatic wave potential normalized by

*m*with

_{e}c^{2}/e*e*being the magnitude of the charge of an electron, the time variable (t) is normalized by ω

_{pi}=(4

*πn*)

_{0}e^{2}/m_{i}^{1/2}and the space variable (

*x*) is normalized by

*λ*=(

_{m}*m*/4

_{e}c^{2}*πn*)

_{0}e^{2}^{1/2}. The coefficient of viscosity

*η*is a normalized quantity given by

*ω*, and

_{i}λ^{2}_{mi}m_{s}n_{so}*α*is the ratio of the number density of electron and ion (

_{e}*n*) and

_{e}/n_{i}*α*is the ratio of the number density of positron and ion (

_{p}*n*). The constants

_{p}/n_{i}*K*

_{1}=

*n*and

_{0}^{α-1}K_{i}/m_{i}^{2}C_{i}^{2}*K*

_{2}=

*n*. The equations of state used here for the degenerate pressures of electrons, ions and positrons are given by

_{0}^{γ-1}K_{e}/m_{i}C_{i}^{2}=n_{0}^{γ-1}K_{p}/m_{i}C_{i}^{2}for the non-relativistic limit (where Λ_{c} = *πћ ^{2}/mc* = 1.2 × 10

^{-10}cm, and

*ћ*is the Planck constant divided by 2

*π*).

While for the electron fluid,

and while for the positron fluid

where for non-relativistic limit [33-35,40,42]

and for the ultra-relativistic limit [33-35,40,42]

**Derivation of Burgersʼ equation**

Now we derive a dynamical equation for the nonlinear propagation of the dust-ion-acoustic shock waves by using (1 - 5). To do so, we employ a reductive perturbation technique to examine electrostatic perturbations propagating in the relativistic degenerate dense dusty plasma due to the effect of dissipation, we first introduce the stretched coordinates [47]

where *V _{p}* is the wave phase speed (

*ω /κ*with

*ω*being angular frequency and

*κ*being the wave number of the perturbation mode), and ∈ is a smallness parameter measuring the weakness of the dispersion (0 < ∈ < 1). We then expand

*n*, and

_{i}, n_{e}, u_{i}*Φ*, in power series of ∈:

and develop equations in various powers of ∈. To the lowest order in ∈, using equations (12)-(18) into equations (1)-(5) we get as, and , where and . The relation represents the dispersion relation for the ion-acoustic type electrostatic waves in the degenerate plasma under consideration. We are interested in studying the nonlinear propagation of these dissipative dust-ion-acoustic type electrostatic waves in a three components degenerate plasma. To the next higher order in ∈, we obtain a set of equations

Now, combining (19-23) we deduce a Burgers^{2} equation

where the value of A and C are given by

The shock wave solution of (24) is

where the special stretched coordinates, *ξ = ζ - u _{0}τ*, the amplitude,

*Φ*the width,

_{m}= u_{0}/A*δ = 2C/u*is the wave speed and the parameter

_{0}, u_{0}*η*was chosen from standard value [48] for the system under consideration.

**Numercial analysis**

We have numerically solved the Burgersʼ equation(24), and have studied the effects of *η, α _{e}*, and

*α*with

_{p}*ξ*on dust-ion-acoustic nonlinear structures of shock waves in both non-relativistic and ultra-relativistic degenerate electrons and positrons where ions always being non-relativistic degenerate. It is obvious from figures 1-12 that the degenerate plasma system under consideration supports compressive and reductive DIA ShWs which are associated with both positive and negative potential and the amplitude of these nonlinear structures of shock waves depends on the Chandrasekhar limits [33], i.e. non-relativistic and ultra-relativistic limits.

In figures 1-6 we have observed the effect of *η, α _{e}, α_{p}*, and

*μ*on the potential structure with the variation of

*ξ*in case of both non-relativistic and ultra relativistic limits. It has been observed when the values of

*μ*is smaller than 0.82 (

*μ*< 0.82) then we observe the formation of positive potential for the nonlinear structures of compressive shock wave in our considered degenerate plasma system. Again we consider the values of

*μ*is greater than or equal to 0.82 (

*μ*> 0.82) then we observe the negative potential for the nonlinear refractive structures as shown in figures from 7 to 12. It should be noted here that in both cases we keep all the parameters same so that it could be easy to analysis the effects of every parameter. The interesting point is that with the increasing values of

*α*and

_{p}*α*, the values of potential increases smoothly, but the increasing values of

_{e}*η*the potential decreases smoothly. It should be noted that the formation of the compressive dust-ion-acoustic shock waves depends only on the values of the ratio of the electron number density and the ion number density (

*α*) and does not depend on the values of

_{e}*α*(the ratio of the electron number density and the positron number density). And the figures 1-12 also show us that the potential for electron-positron (e-p) being ultra-relativistic and ion (i) being non-relativistic degenerate is always greater than for electron-ion-positron (e-i-p) being non-relativistic degenerate.

_{p}From the study of the negative potential in our three components degenerate plasma system, we have observed that with the increasing value of *η* the potential also increases. But it has been also noted that with the increasing values of *η* the potential, (*Φ*^{(1)}) also decreases very smoothly in both limits from figures 7 to 12. It should be noted here that in this case, the values of *μ* is always greater than or equal to 0.82 (*μ* > 0.82). It needs to be pointed here that the formation of the reductive DIA ShWs (shown in figures 7 to 12) depends only on the values of the ratio of the dust number density and the ion number density (*μ*) and does not depend on the values of *α _{e}* and

*α*(the ratio of the number density of electron and ion and the ratio of the positron number density and ion). From the analysis of the negative potential structures for

_{p}*μ*≥ 0.82 (shown in figures 7 -12) it has been again pointed out that the potential for electron-positron (e-p) being ultra-relativistic and ion (i) being non-relativistic degenerate is always greater than for electron-ion-positron (e-i-p) being non-relativistic degenerate.

The profiles of shock wave, caused by the balance between nonlinearity and dissipation, are depicted in figures 1-12. And the potential of the dust-ion-acoustic shock waves profiles for non-relativistic degenerate ions fluid and ultra-relativistic degenerate electrons and positron fluid is different from that when all the particles follow the same limit. From the mathematical calculation and the numerical solution of Burgersʼ equation we have found that for a certain value of *μ* we get both positive and negative potential when all other parameters are kept same, i.e. when the values of *μ* is always less than 0.82 (*μ* < 0.82) then we obtain positive potential and when the values of *μ* is greater than or equal to 0.82 (*μ* ≥ 0.82) then we obtain negative potential. It has made the great interest in the study of the dust-ion-acoustic nonlinear structures of shock waves in an unmagnetized degenerate dense plasma system to analysis the existence conditions for the positive and negative potential where the elements electrons, ions, and positrons are always being degenerate.

It is to be noted here that we have taken all the parameters in normalized form, so all the ranges of parameters are taken arbitrarily.

Discussion

We have considered an unmagnetized degenerate dense plasma containing non-relativistic degenerate cold ions fluid, both non-relativistic and ultra-relativistic degenerate electrons and positrons fluid, and negatively charged dust grains. We have examined the basic features of the electrostatic nonlinear structures that are found to exist in such degenerate dense plasma. In our present investigation all the degenerate constitutes of the considered dense unmagnetized plasma system follow relativistic limits of pressure. The nonlinear DIA shock waves and its propagation have been described thoroughly with Burgersʼʼ equation (24) and itʼs solution (27). The effects of different plasma parameters on the nonlinear propagation of DIA shocks waves have been graphically shown (Figures 1-12).

Our present investigation is different from the related Investigations [40-43,49,50] in the way that we have considered the pressure of all the constituent particle (electrons and ions), as the whole system is degenerate and all the particles should follow the equation of state [6-11] whatever the limit is (non relativistic or ultra-relativistic). This is obvious that the shock profiles obtained from our present investigation are also quite different from the previous investigation [40-42,49,51] in the sense that we have had electrostatic shock profiles while the others have got to support electrostatic solitary profiles [40-42] and double layers [40,41]. The degenerate dense plasma is found to support shock structures whose basic features dependent on the plasma number density. From this point of view our present investigation is more acceptable and the system constituents havemade the validity of our investigations unique.

We note that in our numerical analysis we have used a wide range of the degenerate plasma parameters [33,40,42,49,52,53], which are relevant for many cosmic environments and compact astrophysical objects. The results of the present investigation is, therefore, expected to be useful in understanding the dispersion properties of the electrostatic shock waves in such cosmic environments [14,16,23], compact astrophysical objects [17,18,29] and interstellar compact objects [44,45]. The electrostatic waves in an ultra-relativistic and non-relativistic degenerate dense plasma, which is relevant to interstellar compact objects like white dwarfs, have been investigated. The results, which have been found from this investigation, represent ion acoustic-type of electrostatic waves in which the restoring force comes from the electron-ion degenerate pressure and inertia is provided by the ion mass density.

It can be expected that the basic features and the underlying physics of the DIA shock waves with the existence conditions for positive and negative potential, that have been presented in our present work should be verified by further laboratory experiments. It may also be added here that our investigation is valid for small amplitude DIA shock waves and for unmagnetized and uniform degenerate dense plasma system. These results may be useful to explain some aspects of shock waves in dense e-p-i degenerate plasma. However, arbitrary amplitude DIA shock waves in uniform/nonuniform degenerate dense plasma with or without the external magnetic field are also problems of recent interest for many space and laboratory dusty plasma situations, but beyond the scope of our present investigation. Although such plasma cannot be produced in a laboratory, yet they are gaining considerable attention of the researchers working on degenerate dense astrophysical plasma and numerical simulations. We hope that our present investigation will be helpful for understanding the basic features of the localized electrostatic disturbances in compact astrophysical objects (e.g. white dwarfs, neutron stars, black hole, etc.).

Acknowledgments

P. Halder is profoundly grateful to the Ministry of Science and technology (Bangladesh) for awarding the National Science and Technology (NST) fellowship.

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