Traveling wave solutions of conformable time-fractional Zakharov–Kuznetsov and Zoomeron equations
Introduction
Any phenomenon that changes with respect to time can be modeled by partial differential equations. In real life, we see that the relation between variables are not always linear, so nonlinear models are used to describe the phenomena. Recently, to construct more accurate models, fractional order differential equations have become to use more often. In fact, fractional derivatives have appeared in the late 17th century [1]. Due to the applications in mathematical physics, chemistry, bioengineering, nonlinear optics, optical fibers, control theory, finance, solid mechanics, signal processing and so on, fractional differential equations have take more and more attention. Various derivative definitions from different point of view such as Caputo, Grunwald–Letnikov, Riemann–Liouville and Riesz fractional derivative have been introduced so far [2], [3], [4], [5]. It is known that there are some setbacks of one definition to another and all definitions of fractional derivatives do not satisfy the product, quotient or chain rules. Recently, Khalil et al. [6] introduced a novel definition for fractional derivative to overcome some deficiencies of existing definitions. The proposed definition is called conformable fractional derivative and satisfies product and quotient rules. Also, Abdeljawad [7] contributed this derivative by presenting left and right conformable fractional derivative, fractional integration by parts formulas and chain rule. Atangana et al. [8] gave some new properties of the conformable derivative.
To find analytical solutions of partial and fractional order differential equations numerous methods have been proposed and applied so far [9], [10], [11], [12], [13], [14], [15], [16], [17], [18], [19], [20]. Among them, the trial equation method has been proposed by Liu [21], [22], [23] to investigate the exact solutions of differential equations by reducing the considered equation to solvable differential equation. Some authors [24], [25], [26], [27] applied the trial equation and the modified trial equation methods to some partial differential and fractional differential equations.
In this work, traveling wave solutions of conformable time-fractional differential equations have been investigated. To this aim, we first consider the conformable time-fractional Zakharov–Kuznetsov equation which illustrates the ion-acoustic waves of the weakly nonlinear type in strongly magnetized lossless plasma [28], [29]. The equation was first introduced by Zakharov and Kuznetsov [28]. Till now, some authors [30], [31], [32] applied exp-expansion method, the modified simple equation method, the first integral method, and the modified Kudryashov method to investigate exact solutions of the equation.
We then consider the conformable time-fractional Zoomeron equation which was introduced by Calogero and Degasperis [33]. In the literature, (G’/G)-expansion method, the extended tanh method, the exp-function method, the sub-equation method, the generalized Kudryashov method and exponential rational function technique have been applied to this equation by some authors [34], [35], [36], [37], [38], [39].
This paper implemented the modified trial equation method to the conformable time-fractional Zakharov–Kuznetsov equation and the conformable time-fractional Zoomeron equation for the first time. By means of the method and the complete discrimination system, exact traveling wave solutions including solitary wave solutions, hyperbolic function solutions, and periodic solutions of these equations were successfully obtained. These equations play an important role in mathematical physics, so finding comprehensive analytical methods to solve them will be useful to understand the physical behavior.
Section snippets
Conformable fractional derivative (CFD)
The CFD was defined by Khalil et al. [6] as follows:
Definiton: Suppose that f: [0, ∞) → is a function. Then, the conformable time-fractional derivative of f of order α is
for all t > 0 and α ∈ (0,1).
Some useful properties of the conformable fractional derivative were given with theorems [6], [7], [8].
The modified trial equation method
The method can be described as follows [23]:
Step1. Consider time fractional partial differential equationIntroducing the wave transformationreduces Eq. (1) to a nonlinear ordinary differential equation of integer order as follows:
Step 2. The trial equation can be taken aswhere F(U) and G(U) are polynomials. Putting the Eqs. (4) and (5) into Eq.(3) gives an equation
(3+1)-dimensional conformable time-fractional Zakharov–Kuznetsov (FZK) equation
Consider the FZK equation in the form [28], [29], [30], [31]:The (3+1)-dimensional FZK equation plays a significant role in mathematical physics. The equation describes weakly nonlinear wave process in dispersive and isotropic media such as water waves in shear flows or waves in magnetized plasma [32].
Using the transformationEq. (9) change into the form of an ordinary differential equation (ODE):
Conclusion
The modified trial solution method is implemented for conformable time-fractional differential equations. By using the conformable fractional derivative and the wave transformation, conformable time-fractional partial differential equations have been reduced to the ordinary differential equations. By applying the method and the complete discrimination system, exact traveling wave solutions including periodic solutions, solitary wave solutions, and hyperbolic function solutions of the
ORCID
Meryem Odabasi https://orcid.org/0000-0002-3025-3063
Declaration of Competing Interest
None.
Acknowledgment
This research is supported by Ege University, Scientific Research Project(BAP), Project Number: 17-TKMYO-002.
The authors would like to thank to the editor and the referees for their valuable contributions and comments to improve the paper.
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