Complexity
Volume 2020 (2020), Article ID 2394030, 13 pages
https://doi.org/10.1155/2020/2394030

Research Article

Computational and Numerical Solutions for -Dimensional Integrable Schwarz–Korteweg–de Vries Equation with Miura Transform

Raghda A. M. Attia,1,2 S. H. Alfalqi,³ J. F. Alzaidi,³ Mostafa M. A. Khater,1,4 and Dianchen Lu¹

¹Department of Mathematics, Faculty of Science, Jiangsu University, Zhenjiang 212013, China
²Department of Basic Science, Higher Technological Institute, 10th of Ramadan 44634, Egypt
³Department of Mathematics, Faculty of Science and Arts in Mahayil Asir, King Khalid University, Abha, Saudi Arabia
⁴Department of Mathematics, El Obour Institutes, Cairo 11828, Egypt

Correspondence should be addressed to Mostafa M. A. Khater; mostafa.khater2024@yahoo.com

Received 3 June 2020; Accepted 23 July 2020; Published 14 September 2020

Academic Editor: Alina Gavriluţ

Copyright © 2020 Raghda A. M. Attia et al. 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.

Abstract.

This paper investigates the analytical, semianalytical, and numerical solutions of the –dimensional integrable Schwarz–Korteweg–de Vries (SKdV) equation. The extended simplest equation method, the sech-tanh method, the Adomian decomposition method, and cubic spline scheme are employed to obtain distinct formulas of solitary waves that are employed to calculate the initial and boundary conditions. Consequently, the numerical solutions of this model can be investigated. Moreover, their stability properties are also analyzed. The solutions obtained by means of these techniques are compared to unravel relations between them and their characteristics illustrated under the suitable choice of the parameter values.

1. Introduction

The Korteweg–de Vries (KdV) equation is a seminal model in fluid mechanics. This model was introduced by Boussinesq in 1877 and reintroduced by Diederik Korteweg and Gustav de Vries in 1895. The KdV has the following formula [1–9]:

where characterizes the weakly nonlinear shallow water waves. Equation (1) can be written in many distinct forms and combined with other models. One of them is the Schwarz–Korteweg–de Vries (SKdV) equation given by

where is the unknown function. The SKdV was derived by Krichever and Novikov [10] and Weiss [11, 12].

In this paper, we study the -dimensional integrable generalization of SKdV as follows:

Equation (3) was derived by Toda and Yu [13]. Using the following transformation on equation (3),

where , and are the unknown functions, we obtain

This equation is obtained from the study by Bruzón et al. [14–16]. Using the Miura transform [17–19] on equation (5) as

we obtain [20, 21]

If we adopt the wave transformation

then we convert equation (7) into an ordinary differential equation (NLODE). The integration of the obtained NLODE with zero constant of integration leads to

If we consider the substitution , then it results in

Having these ideas in mind, this paper is organized as follows: Section 2 presents the two methods and derives the solutions of the SKdV equation. Section 5 represents the solutions for several numerical values of the parameters. Additionally, their stability and properties are also discussed. Finally, Section 6 summarises the main conclusions.

2. Explicit Solutions

In this section, we apply two analytical techniques for deriving the solutions of the -dimensional integrable SKdV model. We adopt the extended simplest equation method and the sech-tanh method to obtain various distinct formulas of solitary wave solutions of equation (3). For further details about the two methods, see [22–26].

2.1. Extended Simplest Equation

According to the homogeneous balance rule between the highest derivative and the nonlinear term in equation (9), we obtain . Thus, the general solution of equation (10) is given by

where are arbitrary constants. Additionally, satisfies the following ordinary differential equation:

where are the arbitrary constants. Substituting equations (11) and (12) into (9) and collecting all terms of , we get a system of algebraic equations. Solving this system, we obtain two families of solutions.

Family 1.

Family 2.

From these two families, the solitary wave solutions of equation (7) can be obtained.
According to Family 1, we have the following expressions.

2.1.1. When

For , we obtain

For , we obtain

When , we obtain

According to Family 2, we have the following expressions.

2.1.2. When

For , we obtain

For , we obtain

When : For , we get

For , we obtain

When , we obtain

2.2. Sech-Tanh Method

The general solution of equation (10) according to the sech-tanh method and calculated value of balance is given by

where are the arbitrary constants. Substituting equation (29) into (10) and collecting all terms of , we obtain a system of algebraic equations. Solving this system, we obtain

Consequently, the explicit solution of equation (7) is given by

3. Stability Investigation

We now examine the stability property for -dimensional integrable SKdV model with the Miura transformation by means of an Hamiltonian system. The momentum in the Hamiltonian system is given by

where is the solution of the model. Consequently, the condition for stability of the solutions can be formulated as

where is the wave velocity. The momentum in the Hamiltonian system for equations (18) and (31) are given, respectively, by

And thus,

We conclude that this solution is stable on the interval . This result shows the ability of the solutions for their application. Using the same steps, we can check the stability property of all other obtained solutions.

4. Semianalytical and Numerical Solutions

This section applies semianalytical and numerical schemes for deriving the solutions of the -dimensional integrable SKdV model. The Adomian decomposition method and cubic b-spline schemes are employed to the method to investigate the accuracy of the obtained analytical solutions. Also, this study aims to give a comparison between both used analytical schemes. For further details about the two methods, see [27–30].

4.1. Adomian Decomposition Method

Applying this scheme gives equation (10) in the following form:

Thus, with respect to equation (18) and the following conditions , we obtain

Consequently, the semianalytical solution of equation (10) is written in the following form:

However, with respect to equation (31) and the following conditions , we obtain

Consequently, the semianalytical solution of equation (10) is written in the following form:

4.2. Cubic B-Spline Scheme

Employing the cubic B-spline scheme to evaluate the numerical solutions of equation (10). Using same initial and boundary conditions with respect to the obtained solutions (18) and (31), yields

5. Discussion

This section illustrates several of the results for to highlight the properties of the -dimensional integrable SKdV model with Miura transformation. In the follow-up, we fix the value of to characterize these solutions and the interpretation is based on three different types of representations (three- and two-dimensional charts and contour plot). In the following steps, the physical interpretation of the represented figures is discussed:

(i)Figure 1 shows the bright solitary for (18) in the three-dimensional plot (a) to illustrate the perspective view of the solution, the two-dimensional plot (b) to present the wave propagation pattern of the wave along - axis, and the contour plot (c) to explain the overhead view of the solution when (ii)Figure 2 shows the dark solitary for (31) in the three-dimensional plot (a) to illustrate the perspective view of the solution, the two-dimensional plot (b) to present the wave propagation pattern of the wave along the -axis, and the contour plot (c) to explain the overhead view of the solution when (iii)Figure 3 illustrates the exact and semianalytical obtained solutions, respectively, by the extended simplest equation method and Adomian decomposition method(iv)Figure 4 illustrates the exact and semianalytical obtained solutions, respectively, by the sech-tanh expansion method and Adomian decomposition method(v)Figure 5 illustrates the exact and numerical obtained solutions, respectively, via the sech-tanh expansion method and cubic B-spline scheme(vi)Figure 6 illustrates the exact and numerical obtained solutions, respectively, via the sech-tanh expansion method and cubic B-spline scheme Now, we shall show the accuracy of our obtained solution and explain the comparison between the two employed analytical schemes:(vii)Tables 1 and 2 show calculated values of the exact, semianalytical, and numerical solutions with different values of . These values show the accuracy of the obtained analytical solutions via the sech-tanh expansion method over the obtained analytical solutions via the extended simplest equation method where the absolute values of error in the sech-tanh method is smaller that those obtained by the extended simplest equation method. Figure 7 explains the absolute value of error in 1 and 2.

(a)

(b)

(c)

Figure 1: Solitary wave in three different forms of equation (18).

(a)

(b)

(c)

Figure 2: Solitary wave in three different forms of equation (31).

(a)

(b)

(c)

Figure 3: Exact and numerical solutions of equation (10) according to the obtained analytical solution via the extended simplest equation method.

(a)

(b)

(c)

Figure 4: Exact and numerical solutions of equation (10) according to the obtained analytical solution via the sech-tanh expansion method.

(a)

(b)

(c)

Figure 5: Exact and numerical solutions of equation (10) according to the obtained analytical solution via the extended simplest equation method.

(a)

(b)

(c)

Figure 6: Exact and numerical solutions of equation (10) according to the obtained analytical solution via the sech-tanh expansion method.

(a)

(b)

Figure 7: Absolute value of error via the Adomian decomposition method (a) and cubic B-spline scheme (b) based on the shown value in Tables 1 and 2.

Table 1: Exact, semianalytical, and absolute values of error with different values of with respect to the obtained solution via extended simplest equation method (18) and sech-tanh method (31) via the Adomian decomposition method.

Ext. Sim Eq. method
Sech-tanh method
Absolute error

Value of 3
Exact
Approximate
Exact
Approximate
First scheme
Second scheme

0.001
1.99998
1.99999
0.499999
0.499999
1.19999E−05
4.99711

0.002
1.9999
1.99995
0.499994
0.499994
0.000047999
7.99988

0.003
1.99978
1.99989
0.499987
0.499987
0.000107995
4.05003

0.004
1.99962
1.99981
0.499976
0.499976
0.000191984
1.28001

0.005
1.9994
1.9997
0.499963
0.499963
0.00029996
3.12502

0.006
1.99914
1.99957
0.499946
0.499946
0.000431917
6.48006

0.007
1.99882
1.99941
0.499927
0.499927
0.000587846
1.20052

0.008
1.99846
1.99923
0.499904
0.499904
0.000767738
2.04804

0.009
1.99806
1.99903
0.499879
0.499879
0.00097158
3.28057

0.01
1.9976
1.9988
0.49985
0.49985
0.00119936
5.00013

Table 2: Exact, numerical, and absolute value of error with different value of with respect to the obtained solution via the extended simplest equation method (18) and sech-tanh method (31) via the cubic B-spline scheme.

Value of
Ext. Sim Eq. Method
Sech-tanh method
Absolute error

Exact
Numerical
Exact
Numerical
First scheme
Second scheme

0
−2
−2
−0.5
−0.5
0
0

0.001
−1.99999
−1.99987
−0.499999
−0.499998
0.00012596
8.99958

0.002
−1.99998
−1.99971
−0.499994
−0.499994
0.000263919
1.59986

0.003
−1.99995
−1.99953
−0.499987
−0.499987
0.000413876
2.09974

0.004
−1.9999
−1.99933
−0.499976
−0.499976
0.000575829
2.39971

0.005
−1.99985
−1.9991
−0.499963
−0.499963
0.000749778
2.49963

0.006
−1.99978
−1.99885
−0.499946
−0.499946
0.000935721
2.39959

0.007
−1.99971
−1.99857
−0.499927
−0.499927
0.00113366
2.09953

0.008
−1.99962
−1.99827
−0.499904
−0.499904
0.00134358
1.59955

0.009
−1.99951
−1.99795
−0.499879
−0.499879
0.0015655
8.99764

0.01
−1.9994
−1.9976
−0.49985
−0.49985
0.0017994
0

6. Conclusion

In this paper, the extended simplest equation and sech-tanh expansion methods have been successfully implemented on the -dimensional integrable SKdV model with Miura transform. Moreover, the stability properties of the solutions have also been tackled. The Adomian decomposition method and cubic B-spline scheme have also employed to investigate the semianalytical and numerical solutions, and the two show the accuracy of the obtained analytical solutions. The rigor of the obtained solutions that have been obtained by the sech-tanh expansion method has been discussed. The solutions were represented by allowing a physical interpretation and better interpretation of their properties. In summary, this paper studied the SKdV and found relevant solutions that provide new interpretations of the real-world phenomena.

Data Availability

Data sharing is not applicable for this article as no datasets were generated or analyzed during the current study.

Conflicts of Interest

The authors declare that there are no conflicts of interest.

Authors’ Contributions

All authors conceived the study, participated in its design and coordination, drafted the manuscript, participated in the sequence alignment, and read and approved the final manuscript.

Acknowledgments

The authors extend their appreciation to the Deanship of Scientific Research at King Khalid University, Abha, KSA, for funding this work through the research group under grant number R.G.P-1/151/40.

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