Time-Space Fractional Model for Complex Cylindrical Ion-Acoustic Waves in Ultrarelativistic Plasmas

Liu, Quansheng; Chen, Liguo

doi:https://doi.org/10.1155/2020/9075823

Complexity

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Abstract Introduction Conclusion Data Availability Conflicts of Interest Acknowledgments References Copyright Related Articles

Research Article | Open Access

Volume 2020 | Article ID 9075823 | https://doi.org/10.1155/2020/9075823

Time-Space Fractional Model for Complex Cylindrical Ion-Acoustic Waves in Ultrarelativistic Plasmas

Quansheng Liu¹and Liguo Chen²

Academic Editor: Chongyang Liu

Received20 Nov 2019

Revised11 Mar 2020

Accepted06 Apr 2020

Published22 Apr 2020

Abstract

In this paper, the fractional order models are used to study the propagation of ion-acoustic waves in ultrarelativistic plasmas in nonplanar geometry (cylindrical). Firstly, according to the control equations, (2 + 1)-dimensional (2D) cylindrical Kadomtsev–Petviashvili (CKP) equation and 2D cylindrical-modified Kadomtsev–Petviashvili (CMKP) equation are derived by using multiscale analysis and reduced perturbation methods. Secondly, using the semi-inverse method and the fractional variation principle, the abovementioned equations are derived the time-space fractional equations (TSF-CKP and TSF-CMKP). Furthermore, based on the fractional order transformation, the 1-decay mode solution of the TSF-CKP equation is obtained by using the simplified homogeneous balance method, and using the generalized hyperbolic-function method, the exact analytic solution of TSF-CMKP equation is obtained. Finally, the effects of the phase speed , electron number density (through ) and the fractional order on the propagation of ion-acoustic waves in ultrarelativistic plasmas are analyzed.

1. Introduction

In recent years, plasma physics [1–4] has developed rapidly in the global environment, electromagnetic propagation, and especially in the astronomical environment. In many astronomical environments, matters exist in extremely dense conditions and are not found in the Earth’s environment, and there is a strong interest in understanding the basic properties of matter under extreme dense conditions. In some interstellar dense objects (e.g., white dwarfs and neutron stars), the extreme conditions of matter are caused by the significant compression of the interstellar medium. One of these extreme conditions is the presence of high density degenerate substances in these compact objects. These objects are actually “relics of stars.” They have stopped burning thermonuclear fuel and are no longer able to generate the thermal pressure needed to support the gravitational load of their own mass. These interstellar compact objects are greatly compressed, and their internal density becomes very high. Therefore, the nonthermal pressure is provided by degenerate fermion kinetic energy and particle interactions. This pressure is not sensitive to temperature, i.e., the pressure does not go down as the star cools.

Based on observations and theoretical analysis, there are two types of dense objects that resist gravitational collapse under the action of cold degenerate fermions/electron pressure. An example of the first category is a white dwarf supported by the pressure of degenerate electrons, the interior of which is close to a dense solid (ionic lattice surrounded by degenerate electrons, possibly other heavy particles or dust), and an example of the second category is a neutron star supported by the pressure of nuclear degeneracy and nuclear interaction, which is close to a giant atomic nucleus (mixture of nucleon and electron interactions, possibly other elementary particles and condensates). In such a compact object, the degenerate electron number density is very high. For example, in a white dwarf, the degenerate electron number density can reach the order of , which is expected to be degenerated in a white dwarf of sufficient quality. Electrons become relativistic, making stars prone to gravitational collapse, and the declining electron density in neutron stars can even reach the order of . In the white dwarf and neutron stars, the energy of an electron Fermi is comparable to the energy of an electron resting mass, and the speed of an electron can be comparable to the speed of light in a vacuum [5, 6].

Chandrasekhar [7–9] mathematically explains the equation of state of degenerate electrons in such interstellar dense objects, involving two limits, namely, nonrelativistic and ultrarelativistic limits. The degenerate electron equation of state of Chandrasekhar [7–9] is used viz. (nonrelativistic limit) and (ultrarelativistic limit), where is the degenerate electron pressure and is the degenerate electronic number density. We note that the degenerate electron pressure is only related to the electron number density and not to the electron temperature. These close interstellar objects provide us with a cosmic laboratory that studies the properties of matter (materials) and the fluctuations and instability in a state of extreme density degradation in such media. This has led to the study of linear and nonlinear ion-acoustic wave properties in ultrarelativistic plasmas.

Ion-acoustic waves [10–12] are one of the basic wave processes in plasma. A large number of theoretical and experimental studies have been conducted on ion-acoustic waves for a long time. In the early days, many researchers have extensively studied the nonlinear propagation of ion-acoustic waves in planar geometry [13, 14], such as the Korteweg–de Vries (KdV) equation [15] to describe the propagation of ion-acoustic waves in a one-dimensional plane geometry in plasma. However, for some practical situations such as astronomical environment, laboratory, and space plasma, there is a clear deficiency in one-dimensional planar geometry. Therefore, many scholars have begun to study the propagation of solitary waves in nonplanar cylindrical geometry. For example, Mamun [16] used modified Korteweg–de Vries (mKdV) equation to study the propagation of solitary waves in nonplanar geometry in dust plasma. Mushtaq [17] found that quantum correction and lateral perturbation in cylindrical geometry have effects on solitary wave propagation.

The calculus invented by Newton and Leibniz is a watershed between modern mathematics and classical mathematics. Fractional calculus [18, 19] is a theory of arbitrarily order differential and integral, and it is uniform with integer calculus and is a generalization of integer calculus. For centuries, the theoretical study of fractional calculus has been very limited, mainly in the field of mathematics. For example, Euler, Liouville, Riemann, and Caputo all contribute significantly to the field of fractional calculus. Most of them first introduce fractional order integrals and define fractional derivatives on this basis. However, after a series of improvements, the concept of fractional derivatives [20–22] is more suitable for the modeling of practical problems than the integer derivatives. Fractional differential equations [23–25] are also beginning to be used to solve problems in the fields of biological systems, thermal systems, and mechanical systems, and their practicality is getting stronger. Scholars pay great attention to the fractional calculus theory, especially the fractional differential equations abstracted from practical problems. Fractional calculus has attracted more and more scholars’ research interest. Compared with the integer order model, the fractional order model can better describe the dynamic response of the actual system, improve the performance of the dynamic system, and solve practical problems. However, in the research of plasma physics, most of the models are established in integer order [26, 27]. This makes it necessary to establish a fractional order model to describe and study the propagation of solitary waves in plasma.

With the continuous development of the research on fractional differential equations [28–30], the solution of fractional differential equations becomes an important subject. The solution of fractional equations is the key means to solve and analyze the problem. At present, based on the method of solving integer differential equations [31–34], there are many methods for calculating the exact solutions and numerical solutions of fractional differential equations, such as -expansion method [35, 36], the first integral method [37], method [38], and Hirota bilinear method [31].

The rest of the paper is organized as follows. In Section 2, based on the control equations, the multiscale analysis and perturbation expansion method [39] are used to derive the CKP equation and CMKP equation of integer order. In Section 3, applying the semi-inverse method and the fractional variational principle [40], the integer order equations (CKP and CMKP) are, respectively, transformed into time-space fractional equations (TSF-CKP and TSF-CMKP). In Section 4, based on the fractional order transformation, the exact solutions of the TSF-CKP and TSF-CMKP equation are obtained by using the simplified homogeneous balance method [41] and the generalized hyperbolic-function method [42], respectively. In Section 5, the effects of the phase speed , electron number density (through ), temperature ratio , and fractional order value on the ion-acoustic waves propagation in ultrarelativistic plasmas are studied.

2. Construct of Integer Order Models

We consider the nonlinear propagation of ion-acoustic waves in ultrarelativistic plasmas. In order to better deal with the problems studied, we made the necessary assumptions: the plasma model studied has no external magnetic field effect, i.e., unmagnetized and no collision effect, i.e., collisionless. The plasma studied in this paper consists of two parts: warm ions and ultrarelativistic degenerate electrons. At equilibrium, the electrical neutral condition is , where is the undisturbed ion number density and is the undisturbed electron number density. Assuming that the electron fluid follows the equation of state in this form , the nonlinear dynamics of the low frequency electrostatic ion-acoustic waves in such an ultrarelativistic degenerate dense plasma in 2D cylindrical geometry can be described by the following set of normalized equations:where is the ratio of ion temperature to Fermi electron temperature, and is the Fermi electron temperature. , where , is Planck constant divided by , and is the speed of light in a vacuum. The electron number density and ion number density are normalized by , , and are, respectively, the velocity components of the ion-fluid in the direction of and , and they are normalized by the ion-acoustic waves velocity , and where is the ion mass. The electrostatic potential is normalized by , where is the electronic charge. The spatial coordinates are normalized by the Debye radius , the time is normalized by the ion plasma period , where is the Boltzmann constant.

Equation (1) is a complex set of nonlinear equations. In order to study the motion of nonlinear ion-acoustic waves in ultrarelativistic degenerate plasmas with small amplitude, we use the reductive perturbation method to simplify the complex nonlinear equations into differential equations and retain the most important nonlinear part of the original equations. First, expand the independent variables as follows:where is a small parameter characterizing the strength of nonlinearity.

According to equation (2), we have

The dependent variables , and are expanded as follows:

Substituting equations (3) and (4) into equation (1), we obtain the following equations:

According to the different power expansions of , we obtain

The following equations are obtained under the low-order approximation of :

Under the high-order approximation of , we obtain the (2 + 1) dimensional CKP equation, i.e.,where

Next, we use the same method to derive the (2 + 1)-dimensional CMKP equation. The independent expansion is the same as equation (2), and the new perturbation expansion is as follows:

Substituting equations (3) and (12) into equation (1), we obtain the following equations:

Expanding in equation (13) from high to low power, according to the lowest power of , we obtain

According to equation (14), we have

Under the lower power expansion of , we obtain the following equation:

According to equation (16), we have

Under the highest power expansion of , we obtain

Substituting equations (17) and (18) into equation (16), we obtain the following differential equation:

According to equations (17) and (19), we obtain the (2 + 1)-dimensional CMKP equation, i.e.,where

3. Derivation of Time-Space Fractional Cylindrical Equations

In Section 2, we derive a series of differential equations of integer order. However, with the development of scientific research, compared with the fractional model, the integer order model has obvious shortcomings in describing practical problems. Fractional calculus and fractal calculus have become the hotspots in the fields of mathematics, physics, and engineering. In order to further study the nonlinear propagation of ion-acoustic waves in ultrarelativistic plasmas plasma, in this section, we use the semi-inverse method and fractional variation principle to derive the space-time fractional order equations from equations (10) and (20).

Definition 1 (see [43]). Jumarie’s modified Riemann–Liouville derivative of order is defined asSome properties of the modified Riemann–Liouville derivative are as follows:According to equation (20), we havewhere the coefficients refer to equation (20).
Equation (24) can be rewritten as follows:where is the fractional integral of and is invariant in the process of deriving fractional order equations using the semi-inverse method and the fractional variational principle, so it is omitted in the following derivation process.
Assuming , where is a potential function, and substituting it into equation (25), we obtain the potential equation as follows:Then, the function of equation (26) can be written aswhere are Lagrangian multipliers which can be obtained later.
Applying integration by parts to equation (27) and taking , we haveUsing the variation of equation (28), integrating each term by parts and applying the variation optimum condition, we obtainEquation (29) is equivalent to equation (26), by comparing the coefficients, we obtain the Lagrangian multiplier , i.e.,According to equation (30), the Lagrangian form of equation (25) is as follows:Similarly, the Lagrangian form of the fractional form of equation (25) is given bywhere .
Therefore, we obtain the function of the fractional form of equation (25):According to Agrawal’s method [44], equation (33) changes to the following form:Applying the following fractional integration by parts [44],we obtain the following equation:Optimizing the variation equation (38) and taking , we obtain the Euler–Lagrange equation asSubstituting equation (32) into equation (37), we haveTo find the fractional derivative of the independent variable on both sides of equation (38), we haveLetting and substituting it into equation (39), we obtainTherefore, we obtained the TSF-CMKP equation as follows:Similarly, using the semi-inverse method and fractional variation principle, the TSF-CKP equation can be derived as follows:

Remark 1. When , equations (41) and (42) are the integer order equations. In some cases, we can think of integer order equations as a special case of fractional order equations. Therefore, the fractional model can better describe the nonlinear propagation of ion-acoustic waves in ultrarelativistic plasmas.

4. Solutions of TSF-CKP Equation and TSF-CMKP Equation

In order to better explain the physical phenomena represented by fractional differential equations, it is necessary to obtain exact or numerical solutions of fractional differential equations. In this section, first of all, fractional derivatives are transformed into classical derivatives by fractional transformations. Secondly, we obtain the 1-decay mode solution of TSF-CKP equation by using the simplified homogeneous balance method [41]. Finally, using generalized hyperbolic-function method [42], the exact analytic solution of TSF-CMKP equation is obtained.

4.1. 1-Decay Mode Solution for TSF-CKP Equation

The fractional transforms are introduced as follows [45]:where are constants. Based on the abovementioned transforms, we have

Substituting equation (44) into (41) and taking , we obtainwhere .

We consider the homogeneous balance between and , according to the simplified homogeneous balance method, which means that an undetermined function and its partial derivatives are replaced by a logarithmic function and its derivatives , respectively. Therefore, we suppose that the form of the solution of equation (45) is as follows:where is a constant, is an undetermined function, which can be obtained later, and is a particular solution of equation (45).

Substituting equation (46) into equation (45), since is a particular solution, i.e.,we obtain

Setting the coefficient of be zero, yields , so equation (46) can be rewritten as follows:

Equations (48) and (49) can be simplified as follows:

The function satisfies the homogemeity equation, i.e.,

Equations (49) and (51) are called the nonlinear transformation of equation (45), if is a solution of equation (51), substituting it into equation (49), we obtain the exact solution of equation (45). Next, using the nonlinear transformation, we will find the exact solutions of equation (45).

In view of the homogemeity of (51), we assume that the form of the solution of (51) is as follows:where and can be obtained later.

Substituting equation (52) into equation (51), we obtain

According to equation (53), we obtain an ODE as follows:

Solving equation (54), we havewhere is an arbitrary constant.

Substituting equation (55) into equation (52), we obtain a solution of equation (51):

Substituting equation (56) into equation (46), we obtain an exact 1-decay mode solution of the 2D time-space CKP equation as follows:where

4.2. Exact Analytic Solution for TSF-CMKP Equation

Similarly, based on the fractional transforms of equation (43), we have

Substituting equation (59) into equation (42), we obtainwhere .

Using the generalized hyperbolic-function method, we assume that solutions of equation (60) are the super position of different powers of the sech function, tanh function, and their combinations, i.e.,where , , and are all differentiable functions, while and are determined via the balance of the highest-order contributions in equation (60). Substituting equation (61) into equation (60), along with the simplifications, we havewhere the functions and are both differentiable; supposing that and and equating to zero the coefficients of like powers of , , etc., we obtain

Using this algorithm, we obtain the exact analytical solution of equation (60):where the independent variable satisfies the following transformation:

5. The Property of the Ion-Acoustic Waves in Ultrarelativistic Plasmas

In this section, in order to further understand the propagation characteristics of ion-acoustic waves in astrophysical ultrarelativistic degenerate plasmas (especially in white dwarfs and neutron stars). Based on exact analytical solutions, we have studied the effects of the phase speed and electron number density (through ) on the propagation of ion-acoustic waves in astrophysical ultrarelativistic degenerate plasmas. In particular, due to the establishment of fractional order models, we studied the effect of fractional order on the propagation of ion-acoustic waves, which is rare in previous studies.

5.1. Study of the Effects of Electron Number Density (through ) on Ion-Acoustic Waves Propagation

First, we take the variable T as the determined value and draw the figures of the ion-acoustic waves under the axis of the independent variables and .

As shown in Figure 1, within a certain value range, as the value of increases, the peak of the ion-acoustic wave continuously decreases, and eventually the peak almost disappears, and only a valley exists. As the value of increases, the amplitude of the ion-acoustic wave continues to decrease, which indicates that the loudness of the ion-acoustic wave continues to decrease. Therefore, the plasma system makes the ion-acoustic waves damp with the increase of electron number density.

(a)

(b)

(c)

(d)

Then, we take the variable as the determined value and draw the figures of the ion-acoustic waves under the axis of the independent variables and .

As shown in Figure 2, the ion-acoustic waves will undergo radial displacement over time, which is ignored by the one-dimensional model. With the increase of , the trend of the peaks and troughs is the same as that shown in Figure 1. Similarly, the ion-acoustic waves will decay with the increase of .

(a)

(b)

(c)

(d)

5.2. Study of the Effects of the Phase Speed on Ion-Acoustic Waves Propagation

As shown in Figures 3 and 4, it can be concluded that within a certain value range, as the value of the phase velocity decreases, the peak of the ion-acoustic waves continuously decreases, and finally the peak almost disappears, and only a trough exists, and the amplitude of ion-acoustic waves is decreasing. Although the specific change values are different, the trend of this change is similar to the effect of the electron number density on the propagation of ion-acoustic waves, which is precisely because of , so the phase speed also affects the propagation of ion-acoustic waves.

(a)

(b)

(c)

(d)

(a)

(b)

(c)

(d)

5.3. Study of the Effects of the Fractional Order Values on Ion-Acoustic Waves Propagation

Taking the variables and as definite values, Figure 5(a)–5(d) are, respectively, the figures of ion-acoustic waves when the fractional order value is .

(a)

(b)

(c)

(d)

As shown in Figure 5, the properties of peaks, troughs, and amplitudes of ion-acoustic waves are different under different fractional orders, and Figure 5(b) with fractional order value is , which is more special.

Next, we focus on the properties of ion-acoustic waves when the fractional order is and compare it with the case of integer order. Figure 6(a)–6(e) are all the figures when the fractional order is , and Figure 6(f) is the figure when the fractional order is 1, i.e., the figure of integer order.

(a)

(b)

(c)

(d)

(e)

(f)

As shown in Figure 6, when the fractional order value is , as the decreases, the peak first increases and then decreases, the amplitude first increases and then decreases, and the trough gradually decreases. When , the peaks in the integer order figures gradually disappear and a deep trough appears, but the peaks in the fractional figures do not disappear but increase. This reflects the influence of the fractional order values on the ion-acoustic waves in ultrarelativistic plasmas, indicating that it is practical to study the fractional order models in ion-acoustic waves.

6. Conclusion

In this paper, the 2D CKP equation and the 2D CMKP equation in integer order are derived. Compared with the model in one-dimensional plane geometry, the study of models in nonplanar geometry is more in line with the actual situation of the laboratory, space environment, and so on. We extended these equations to the fractional order domain for the first time and obtained the TSF-CKP equation and the TSF-CMKP equation. Compared with the integer order model, the fractional order model can better describe the propagation of ion-acoustic waves in ultrarelativistic plasmas and solve practical problems. Based on the fractional order transformation, the 1-decay mode solution for the TSF-CKP equation is obtained by using the simplified homogeneous balance method, and using the generalized hyperbolic-function method, the exact analytic solution of TSF-CMKP equation is obtained. Next, we use the obtained exact solution to analyze the effects of the phase speed , electron number density (through ), and fractional order on the propagation of ion-acoustic waves in ultrarelativistic plasmas. In particular, the different effects of the fractional order of and 1 on the propagation of ion-acoustic waves are analyzed. These results have potential value for studying the propagation characteristics of ion-acoustic waves in the ultrarelativistic plasmas.

Data Availability

There are no data in our manuscript.

Conflicts of Interest

The authors declare that there are no conflicts of interest regarding the publication of this paper.

Acknowledgments

This work was supported by the National Natural Science Foundation of China (Grant 11562014) and Natural Science Foundation of the Inner Mongolia Autonomous Region (Grant 2017MS0108).

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Copyright © 2020 Quansheng Liu and Liguo Chen. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

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