Mathematics Letters
Volume 1, Issue 1, June 2015, Pages: 1-9

Regarding New Complex Analytical Solutions for the Nonlinear Partial Vakhnenko-Parkes Differential Equation via Bernoulli Sub-Equation Function Method

Haci Mehmet Baskonus1, *, Hasan Bulut2, Dilara Gizem Emir2

1Department of Computer Engineering, Tunceli University, Tunceli, Turkey

2Department of Mathematics, University of Firat, Elazig, Turkey

Email address:

(H. M. Baskonus)
(H. Bulut)
(D. G. Emir)

To cite this article:

Haci Mehmet Baskonus, Hasan Bulut, Dilara Gizem Emir. Regarding New Complex Analytical Solutions for the Nonlinear Partial Vakhnenko-Parkes Differential Equation via Bernoulli Sub-Equation Function Method. Mathematics Letters. Vol. 1, No. 1, 2015, pp. 1-9. doi: 10.11648/j.ml.20150101.11


Abstract: In this research, a structure of the Bernoulli sub-equation function method is proposed. The nonlinear partial Vakhnenko-Parkes differential equation which is another name the reduced Ostrovsky equation has been taken into consideration. Then, analytical solutions such as rational function solution, exponential function solution, hyperbolic function solution, complex trigonometric function solution and periodic wave solution have been obtained by the same method. All necessary calculations while obtaining the analytical solutions have been accomplished through using commercial wolfram software Mathematica 9.

Keywords: The Bernoulli Sub-Equation Function Method, Nonlinear Partial Vakhnenko-Parkes Differential Equation, The Reduced Ostrovsky Equation, Rational Function Solution, Exponential Function Solution, Hyperbolic Function Solution, Complex Trigonometric Function Solution


1. Introduction

Especially, the last two decade have witnessed significant developments of various methods such as Böcklund transformation method, inverse scattering method, the exp-function method, the modified simple equation method, various trial equation methods, Sumudu transform method, the tanh function method, the sine–cosine method, the tanh–sech method, homogeneous balance method, the Darboux transformation, Variable separation approach, Variational iteration method and so on [1-10] for obtaining exact solutions to the nonlinear evolution equations.

In this paper, we have applied the Bernoulli sub-equation function method (BSEFM) [11] to the nonlinear partial Vakhnenko-Parkes equation (NPVPE) [12-24] defined by

(1)

2. General Structure of Approach

In this sub-section, an approach to the NPVPE will be given. In order to apply this method to the NPVPE, we consider the following steps [11].

Step 1. We consider the partial differential equation in two variables such as  and a dependent variable  

(2)

and take the wave transformation

(3)

whereSubstituting Eq.(3) in Eq.(2), it gives us the following  nonlinear ordinary differential equation;

(4)

Step 2. Take trial equation as follows:

(5)

in which

(6)

whereand  is Bernoulli differential polynomial. Substituting above relations in Eq.(4), we obtain an equation of polynomialof

(7)

According to the balance principle, we can get values ofand .

Step 3. Let’s consider the coefficients of  all be zero, we will obtain an algebraic equations system:

(8)

Solving this system, we will determine the values of

Step 4. When we solve nonlinear Bernoulli differential equation Eq.(6) by using methods known, we obtain following two situations according to and ;

(9)

(10)

where Using a complete discrimination system for polynomial to classify the roots of , we solve Eq.(5) with the help of Mathematica 9 programming and classify the exact solutions to Eq.(5). For a better interpretations of results obtained in this way, we can plot two and three dimensional surfaces of analytical solutions obtained by taking into consideration suitable parameter.

3. Implementation of Proposed Method

In this section, we have obtained some new analytical solutions such as rational function, exponential function, hyperbolic function, complex trigonometric function and periodic wave solutions of NPVPE by using BSEFM.

Application First of all, if we perform travelling wave transformation to NPVPE in the following manner;

(11)

(12)

where  is a constant and not zero, we get the nonlinear ordinary differential equation as following;

(13)

Integrating Eq.(13) and considering the constant of integration to be zero, we rewrite the Eq.(13) as following;

(14)

when we reconsider to Eq.(5) and Eq.(6) for balance principle, we obtain following relationship forand

(15)

This resolution procedure is applied and we obtain results as follows:

Case 1: If we take  and  for Eq. (15), then, we write following equations;

(16)

(17)

and

(18)

whereWhen we use Eqs.(16,17,18) in the Eq.(14), we get a system of algebraic equations for Eq.(14). Therefore, we attain a system of algebraic equations from the coefficients of polynomial of. By solving this algebraic equation system for Eq.(16) with the help of Mathematica programming 9, we  obtain the following coefficients;

Case 1a. Forit can be considered that the following coefficients;

(19)

Substituting Eq.(19) in Eq.(16) along with Eq.(3), we obtain the exponential function solution to the NPVPE in the following form;

(20)

Figure 1. The 3D and 2D surfaces of the analytical solution Eq.(20) being exponential function solution by considering the values  for 3D graphics andfor 2D surfaces.

Case 1b. If it is taken asfor Eq.(19), it can be obtained that the following coefficients;

(21)

Substituting Eq.(21) values in Eq.(16) along with Eq.(3),  we obtain another exponential function solution to the nonlinear partial Vakhnenko-Parkes equation in the following manner;

(22)

 

Figure 2. The 3D and 2D surfaces of the analytical solution Eq.(22) being another exponential function solution by considering the values  for 3D graphics andfor 2D surfaces.

Case 1c. For it can be considered that the following coefficients

(23)

Substituting Eq.(23) coefficients in Eq.(16) along with  Eq.(3),we obtain the new hyperbolic function solution for NPVPE in the  following manner;

(24)

 

Figure 3. The 3D and 2D surfaces of the analytical solution Eq.(24) being new hyperbolic function solution by considering the values  for 3D graphics andfor 2D surfaces.

Case 1d. If it is chosen asfor Eq.(23), it can be obtained that the following coefficients;

(25)

Substituting Eq.(25) in Eq.(16) along with Eq.(3),  we obtain the new trigonometric complex function solution of the nonlinear partial Vakhnenko-Parkes equation in the following manner;

(26)

Figure 4. The 3D and 2D surfaces of real part of the analytical solution Eq.(26) by considering the values  for 3D graphics and  for 2D surfaces.

Figure 5. The 3D and 2D surfaces of imaginary part of the analytical solution Eq.(26) by considering the values  for 3D graphics and  for 2D surfaces.

Case 1e. For it can be considered that the following coefficients

(27)

Setting Eq.(27) in Eq.(16) along with Eq.(3), we obtain the new complex exponential function solution to the NPVPE as following;

(28)

 

Figure 6. The 3D and 2D surfaces of imaginary part of the analytical solution Eq.(28) by considering the values  for 3D graphics and  for 2D surfaces.

Figure 7. The 3D and 2D surfaces of real part of the analytical solution Eq.(28) by considering the values  for 3D graphics and  for 2D surfaces.

Case 1f. If it is gotten for Eq.(27), it can be obtained that the following coefficients;

(29)

Substituting Eq.(29) coefficients in Eq.(16) along with Eq.(3), we obtain the another complex trigonometric function solution for the nonlinear partial Vakhnenko-Parkes equation as following;

(30)

Figure 8. The 3D and 2D surfaces of imaginary part of the analytical solution Eq.(30) by considering the values  for 3D graphics and  for 2D surfaces.

 

Figure 9. The 3D and 2D surfaces of real part of the analytical solution Eq.(30) by considering the values  for 3D graphics and  for 2D surfaces.

Case 1g. For it can be considered that the following coefficients;

(31)

Setting Eq.(31) values in Eq.(16) along with Eq.(3),  we obtain the another complex exponential function solution to the NPVPE in the following manner;

(32)

Figure 10. The 3D and 2D surfaces of imaginary part of the analytical solution Eq.(32) by considering the values  for 3D graphics and  for 2D surfaces.

Figure 11. The 3D and 2D surfaces of real part of the analytical solution Eq.(32) by considering the values  for 3D graphics and  for 2D surfaces.

Case 1h. When it is taken into consideration asfor Eq.(31), it can be obtained that the following coefficients;

(33)

Substituting Eq.(33) values in Eq.(16) along with Eq.(3), we obtain the another complex trigonometric function solution for the nonlinear partial Vakhnenko-Parkes equation in the following form;

(34)

Figure 12. The 3D and 2D surfaces of imaginary part of the analytical solution Eq.(34) by considering the values   for 3D graphics and  for 2D surfaces.

 

Figure 13. The 3D and 2D graphs of real part of the analytical solution Eq.(34) by considering the values  for 3D graphics and  for 2D surfaces.

Case 2: If we take  and  for Eq. (15), then, we can write the following equalities;

(35)

and

(36)

where When we put Eqs.(35,36) in Eq.(14), we obtain a system of algebraic equations for Eq.(14). Therefore, we attain a system of algebraic equations from these coefficients of polynomial of. By solving this algebraic equations system with the help of wolfram Mathematica programming 9, we can obtain the following coefficients;

(37)

in which Putting Eq.(37) values in Eq.(35) along  with Eq.(3),  we get the another new exponential rational function solution for the NPVPE in the following manner;

(38)

Figure 14. The 3D and 2D surfaces of the analytical solution Eq.(38) being a new exponential function solution by considering the values  for 3D graphics and  for 2D surfaces.

Remark-1. The solutions  and obtained via BSEFM are the analytical solutions for Eq.(1). When we compare these analytical solutions with other analytical solutions obtained by using different approaches in literature [2],some of these solutions are complex exponential function solutions and new analytical solutions for Eq.(1).

Afterwards, Figure.1, Figure.2, Figure.3, Figure.4, Figure.5, Figure.6, Figure.7, Figure.8, Figure.9, Figure.10, Figure.11, Figure.12, Figure.13 and Figure.14 have been plotted by the same computer program.

To the best of our knowledge, these complex exponential function solutions have not been submitted to literature in advance. The analytical solutions and figures obtained in this paper give us a different physical interpretation for the nonlinear Vakhnenko-Parkes differential equation.

4. Conclusions

BSEFM has been exerted to the nonlinear Vakhnenko-Parkes differential equation. Afterwards, this method has provided us some new analytical solutions such as rational function solution, exponential function solution, and complex trigonometric function solution, periodic wave solution and so on. All analytical solutions obtained by BSEFM in the paper have been controlled whether they are verified to the nonlinear Vakhnenko-Parkes equation with the aid of commercial software Wolfram Mathematica programming 9 and all new solutions has verified to this equation.

It has been observed that solutions gained via the method proposed are in good agreement with already presented informations. Therefore, we think that this method can also be conducted to other nonlinear evaluation equations.


References

  1. J.H. He, Variational iteration method—some recent results and new interpretations, Journal of Computational and Applied Mathematics, 207(1), 3–17, 2007.
  2. X.M Qian, SY Lou, XB Hu. Variable Separation Approach for a Differential difference Asymmetric Nizhnik– Novikov –Veselov Equation, Z Naturforsch A, 59, 645–58, 2004.
  3. H. Bulut, Classification of exact solutions for generalized form of K(m,n) equation, Abstract and Applied Analysis, 2013, 1-11 pages, 2013.
  4. X.M Qian, SY Lou, XB Hu. Variable separation approach for a differential–difference system: special Toda equation,Journal of Physics A: Mathematical and General, 37, 2401–24011, 2004.
  5. C.S. Liu, Applications of complete discrimination system for polynomial for classifications of traveling wave solutions to nonlinear differential equations, Computer Physics Communications, 181, 317-324, 2010.
  6. C.S. Liu, Trial equation method and its applications to nonlinear evolution equations, Acta Physica Sinica, 54, 2505-2509, 2005.
  7. C.S. Liu, A new trial equation method and its applications, Communications in Theoretical Physics, 45, 395-397, 2006.
  8. C.S. Liu, Trial Equation Method to Nonlinear Evolution Equations with Rank In homogeneous: Mathematical Discussions and Its Applications,Communications in Theoretical Physics, 45, 219-223, 2006.
  9. A.Bekir, O. Guner and B. Ayhan, Exact solutions of some systems of fractional differential-difference equations, Mathematical Methods in the Applied Sciences, DOI: 10.1002/mma.3318, 2014.
  10. H. Bulut, H. M. Baskonus, Y. Pandir, The modified trial equation method for fractional wave equation and time-fractional generalized Burgers equation, Abstract and Applied Analysis, 2013, 13 pages, 2013.
  11. B. Zheng, Application of A Generalized Bernoulli Sub-ODE Method For Finding Traveling Solutions of Some Nonlinear Equations, WSEAS Transactions on Mathematics, 7(11), 618-626, 2012.
  12. E. Yusufoğlu, A. Bekir, The tanh and the sine-cosine methods for exact solutions of the MBBM and the Vakhnenko equations, Chaos, Solitons and Fractals, 38, 1126–1133, 2008.
  13. H. Roshid , R. Kabir, Rajandra Chadra Bhowmik and Bimal Kumar Datta, Investigation of Solitary wave solutions for Vakhnenko-Parkes equation via exp-function and Exp(−ϕ(ξ))-expansion method, SpringerPlus, 3(692), 1-10, 2014.
  14. V. O., Vakhnenko, E. J., Parkes, A. J., Morrison, A Böcklund transformation and the inverse scattering transform method for the generalized Vakhnenko equation, Chaos Soliton Fractals, 17(4), 683-692, 2003.
  15. Y. Ye, J. Song, S. Shen, Y. Di, New coherent structures of the Vakhnenko–Parkes equation, Results in Physics, 2, 170–174, 2012.
  16. VO. Vakhnenko High-frequency soliton-like waves in a relaxing medium, Journal of Mathematical Physics, 40, 2011–2020, 1999.
  17. V. O. Vakhnenko and E. J. Parkes, The two loop soliton solution of the Vakhnenko equation, Nonlinearity, 11(6), 1457–1464, 1998.
  18. F., Kangalgil, F., Ayaz, New exact travelling wave solutions for the Ostrovsky equation, Physics Letters A., 372, 1831-1835, 2008.
  19. L. A. Ostrovsky, Nonlinear internal waves in a rotating ocean, Oceanology, 18, 119–125, 1978.
  20. E. Yasar, New travelling wave solutions to the Ostrovsky equation, Applied Mathematics and Computation, 216(11), 3191–3194, 2010.
  21. E. Yusufoglu and A. Bekir, A travelling wave solution to the Ostrovsky equation, Applied Mathematics and Computation, 186(1), 256–260, 2007.
  22. AJ, Morrison, E.J., Parkes, V.O., Vakhnenko, The n loop soliton solution of the Vakhnenko equation, Nonlinearity,12, 427–1437, 1999.
  23. V.O.,Vakhnenko, E.J., Parkes, A.V., Michtchenko The Vakhnenko equation from the viewpoint of the inverse scattering method for the KdV equation, International Journal of Differential Equations and Applications, 1, 429–49, 2000.
  24. V.O., Vakhnenko, E.J., Parkes, The calculation of multi-soliton solutions of the Vakhnenko equation by the inverse scattering method. Chaos, Solitons & Fractals, 13, 1819–1826, 2002.

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