Home Closed-form wave structures of the space-time fractional Hirota–Satsuma coupled KdV equation with nonlinear physical phenomena
Article Open Access

Closed-form wave structures of the space-time fractional Hirota–Satsuma coupled KdV equation with nonlinear physical phenomena

  • Md Nur Alam EMAIL logo , Aly R. Seadawy EMAIL logo and Dumitru Baleanu
Published/Copyright: September 24, 2020

Abstract

The present paper applies the variation of ( G / G ) -expansion method on the space-time fractional Hirota–Satsuma coupled KdV equation with applications in physics. We employ the new approach to receive some closed form wave solutions for any nonlinear fractional ordinary differential equations. First, the fractional derivatives in this research are manifested in terms of Riemann–Liouville derivative. A complex fractional transformation is applied to transform the fractional-order ordinary and partial differential equation into the integer order ordinary differential equation. The reduced equations are then solved by the method. Some novel and more comprehensive solutions of these equations are successfully constructed. Besides, the intended approach is simplistic, conventional, and able to significantly reduce the size of computational work associated with other existing methods.

1 Introduction

Nonlinear dynamical systems play an important role in physics. New ideas in physics including astrophysics, computational physics, fluid dynamic, mathematical physics, biological physics and medical physics often explain the fundamental mechanisms studied by other sciences and suggest new avenues of research in academic disciplines such as mathematics. Nature and research problems and most of the life and compound phenomena are explained and invented through fractional wave models. For example, the fluid-dynamic traffic model [1] could succeed the deficiency based upon the hypothesis of continuum traffic flow, the principles of fractional calculus could model the dynamical methods in fluids and porous structures [2] and fractional derivatives can form the nonlinear oscillation of earthquake [3]. For all the attention, it is an indispensable task to attain the closed-form wave structures of the fractional differential equations (FDEs). Various meaningful and truthful approaches have been interpolated for achieving the closed-form wave structures of FDEs, including the exp ( ϕ ( ξ ) ) -expansion approach [4,5], extended Jacobi elliptic function expansion method [6], improved sub-equation scheme [7], modified fractional reduced differential transform method [8], sub-equation method [9], singular manifold method [10], fractional homotopy method [11], fractional reduced differential transform method [12], modified ( G / G ) -expansion approach [13], extended modified mapping method [14], Sine–Gordon expansion method [15], extended trial equation method [16], iterative method [17], simplest equation method [18], ansatz scheme [19], F-expansion method [20], modified Kudryashov method [21], extended mapping method [22], homo separation analysis method [23], modified simple equation method [24], reduced differential transform scheme [25], modified extended mapping method [26], functional variable method [27], extended direct algebraic method [28], Darcy’s law rule [29], function transformation method [30], the variation of ( G / G ) -expansion method [31], differential transform method [32], unified scheme, ( G / G ) -expansion approach [33,34], Kudryashov method [35], new extended Kudryashov process [36], Sine-cosine approach [37], auxiliary equation scheme [38] and many other techniques [39,40,41,42,43,44,45,46,47,48,49,50].

Here, we introduce a new method [31] for nonlinear FDEs based on the homogenous balancing method employing wave transformation. In this research, through the transformation ξ = k x β Γ ( 1 + β ) + λ t β Γ ( 1 + α ) for ordinary differential equation and ξ = x + y + z V t α α for partial differential equation, a given fractional ordinary and a partial differential equation turn into a fractional ordinary differential equation. Suppose the solutions have the form V ( ξ ) = i = 0 M A i L i + i = 1 M B i L i 1 H , where L = G G , H = N N , where G = G ( ξ ) and N = N ( ξ ) represent the solution of the coupled Riccati equation G ( ξ ) = G ( ξ ) N ( ξ ) and N ( ξ ) = 1 N ( ξ ) 2 . This coupled Riccati equation gives us four types of hyperbolic function solutions, such as sech, tanh, csch and coth. We have manipulated the unique method for obtaining more general closed form wave structures of the nonlinear FDEs, such as the space-time fractional Hirota–Satsuma coupled KdV equation [36]. The improvement of this process over the existing rule is that it presents a few novel closed-form wave solutions. Apart from the physical importance, the closed-form wave structures of the nonlinear FDEs might be helpful to the analytical solvers to compare the exactness of their outcomes and also develop the stability analysis of the nonlinear FDEs. In Section 2, some definitions, characters, properties, theorems and fundamental facts of fractional derivatives are introduced. Section 3 shows that the current scheme of the closed-form wave solutions of the proposed models is obtained in Section 4. Discussion and future works are given in Section 5.

2 Preliminaries

Herein, we acquaint a few definitions, characters, properties, theorems and fundamental facts, which are implemented throughout this article.

2.1 The modified Riemann–Liouville derivative

Fractional calculus possesses several ways to generalize the concept of differential derivatives to fractional derivatives [51,52].

Definition 2.1

A real function g ( t ) , t > 0 is called in the space C k where k if there exists a real number p > k , for example, g ( t ) = t p g 1 ( t ) , where g 1 ( t ) C ( 0 , ) and called in the space C k n if g n C k , where n is a positive integer.

Definition 2.2

Suppose that g : x g ( x ) . It denotes a continuous but not significantly differentiable function, then the fractional derivatives of order α are represented through the following expression [51,52]:

(1) D x α = 1 Γ ( α ) 0 x ( x ξ ) α 1 [ G ( ξ ) G ( 0 ) ] d ξ , α < 0 , 1 Γ ( α ) d d x 0 x ( x ξ ) α [ G ( ξ ) G ( 0 ) ] d ξ , 0 < α < 1 , ( G ( n ) ( x ) ) α m , m α m + 1 , m 1 ,

in which Γ ( . ) is the Gamma function illustrated by [53].

(2) Γ ( α ) = lim m m ! m α α ( α + 1 ) ( α + 2 ) ( α + m )

or

(3) Γ ( x ) = 0 e t t x 1 d x

and

(4) D x α = lim h 0 h α k = 0 ( 1 ) k G [ x + ( α k ) h ] .

Definition 2.3

The Mittag–Leffler function including two parameters is represented as follows [54]

(5) E α , β ( x ) = i = 0 x i Γ ( α i + β ) , Re ( α ) > 0 , β , x C .

Some notable characteristics for the fractional derivative are as follows:

  1. D x α x γ = Γ ( 1 + γ ) Γ ( 1 + γ α ) x γ α , γ > 0 .

  2. D x α ( c G ( x ) ) = c D x α ( G ( x ) ) .

  3. D x α ( a G ( x ) + b H ( x ) ) = a D x α G ( x ) + b D x α H ( x ) .

2.2 The fractional complex transformation

This section performs the complex fractional transformation for the fractional-order ordinary differential equation (ODE). First, we explore the nonlinear fractional ODE:

(6) P ( u , D t α u , D x β u , D t α D t α u , D t α D x β u , D x β D x β u , ) = 0 ,

where 0 < α 0 , 0 < β 0 , D t α u and D x β u are the fractional derivatives of u with respect to t and x.

We investigate equation (6) through the transformation u = u ( x , t ) = u ( ξ ) , ξ = k x β Γ ( 1 + β ) + λ t β Γ ( 1 + α ) , where k and λ are nonzero arbitrary constants, then equation (6) becomes

(7) Q = u , u ξ , 2 u ξ 2 , 3 u ξ 3 , = 0 .

3 Glimpse of the method

At this moment, the general scheme of the variation of ( G / G ) -expansion method [31] is shortened as follows:

  • Step 1: Calculate N through rule of the homogeneous balance in equation (7).

  • Step 2: Considering the method can be expressed as the form:

    (8) V ( ξ ) = i = 0 M A i L i + i = 1 M B i L i 1 H ,

    where L = G G , H = N N and G = G ( ξ ) and N = N ( ξ ) represent the solution of the coupled Riccati equations

    (9) G ( ξ ) = G ( ξ ) N ( ξ ) ,

    (10) N ( ξ ) = 1 N ( ξ ) 2 .

    These coupled Riccati equations give us four types of hyperbolic function solutions including sech, tanh, csch and coth such as

    (11) G ( ξ ) = ± sech ( ξ ) , N ( ξ ) = tanh ( ξ ) ,

    (12) G ( ξ ) = ± csch ( ξ ) , N ( ξ ) = coth ( ξ ) .

  • Step 3: A polynomial in L or N is accomplished plugging equation (8) into equation (7). Determining the coefficients of the equivalent power of L or N produces a system of algebraic equations, which can be determined to construct the values of A i and B i using MAPLE. Turning the over measured values of A i and B i in 12, the general solutions of equation (16) and (17) complete the calculation of the result of equation (6).

4 Implementation of the method

To illustrate the idea of the new method, we implement the process on the space-time fractional Hirota–Satsuma coupled KdV equation. We implement the new method to the considered model, which models the intercommunication between two long waves that have well-defined dispersion connection:

(13) D t α u = 1 4 u x x x + 3 u u x + 3 ( v 2 + w ) x D t α v = 1 2 v x x x 3 u v x D t α w = 1 2 w x x x 3 u w x ,

where u = u ( x , t ) , u = u ( x , t ) and u = u ( x , t ) , t > 0 and 0 < α 0 . For our goal, we utilize the transformations

u ( x , t ) = 1 λ u ( ξ ) 2 , v ( x , t ) = λ + u ( ξ ) , w ( x , t ) = 2 λ 2 2 λ u ( ξ ) ,

where ξ = x λ t β Γ ( 1 + α ) . Then equation (13) reduced to the ODE

(14) λ 2 u ξ 2 + 2 u 3 2 λ 2 u .

Applying the homogeneous balance rule on equation (14) yields M = 2 . Therefore,

(15) u ( ξ ) = ( a 0 b 2 ) + b 1 N ( a 1 + b 1 ) N + ( a 2 + b 2 ) N 2 ,

where a 0 , a 1 , a 2 , b 1 and b 2 are free parameters. Plugging equation (15) into equation (14) and calculating each coefficient of L or N to zeros, we have:

  • Case 1: Let λ = 1 , a 0 = b 2 , a 1 = ± 1 , a 2 = b 2 , b 1 = 0 , and insert the values of Case 1 into equation (15), we find:

    (16) u 1 ( x , t ) = 1 + sech 2 2 x + 2 t α Γ ( 1 + α ) ,

    (17) u 2 ( x , t ) = 1 csch 2 2 x + 2 t α Γ ( 1 + α ) ,

    (18) v 1 ( x , t ) = 1 tanh 2 x + 2 t α Γ ( 1 + α ) ,

    (19) v 2 ( x , t ) = 1 coth 2 x + 2 t α Γ ( 1 + α ) ,

    (20) w 1 ( x , t ) = 2 2 tanh 2 x + 2 t α Γ ( 1 + α ) ,

    (21) w 2 ( x , t ) = 2 2 coth 2 x + 2 t α Γ ( 1 + α ) .

  • Case 2: Let λ = 4 , a 0 = b 2 , a 1 = 4 , a 2 = b 2 , b 1 = 2 and put the values of Case 2 into equation (15), we get:

    (22) u 3 ( x , t ) = tanh 2 2 x + 2 t α Γ ( 1 + α ) + 1 2 tanh 2 2 x + 2 t α Γ ( 1 + α ) ,

    (23) u 4 ( x , t ) = coth 2 2 x + 2 t α Γ ( 1 + α ) + 1 2 coth 2 2 x + 2 t α Γ ( 1 + α ) ,

    (24) v 3 ( x , t ) = 4 + 2 tanh x + 4 t α Γ ( 1 + α ) + 2 tanh x + 4 t α Γ ( 1 + α ) ,

    (25) v 4 ( x , t ) = 4 + 2 coth x + 4 t α Γ ( 1 + α ) + 2 coth x + 4 t α Γ ( 1 + α ) ,

    (26) w 3 ( x , t ) = 32 + 16 tanh x + 4 t α Γ ( 1 + α ) + 16 tanh x + 4 t α Γ ( 1 + α ) ,

    (27) w 4 ( x , t ) = 32 + 16 coth x + 4 t α Γ ( 1 + α ) + 16 coth x + 4 t α Γ ( 1 + α ) .

  • Case 3: Let λ = 1 , a 0 = b 2 , a 1 = 1 , a 2 = b 2 , b 1 = ± 1 and substitute the values of Case 3 into equation (15), we achieve:

    (28) u 5 ( x , t ) = coth 2 2 x + 2 t α Γ ( 1 + α ) ,

    (29) u 6 ( x , t ) = tanh 2 2 x + 2 t α Γ ( 1 + α ) ,

    (30) v 5 ( x , t ) = 1 1 tanh 2 x + 2 t α Γ ( 1 + α ) ,

    (31) v 6 ( x , t ) = 1 1 coth 2 x + 2 t α Γ ( 1 + α ) ,

    (32) w 5 ( x , t ) = 2 2 tanh 2 x + 2 t α Γ ( 1 + α ) ,

    (33) w 6 ( x , t ) = 2 2 coth 2 x + 2 t α Γ ( 1 + α ) .

  • Case 4: Let λ = 4 , a 0 = b 2 , a 1 = 4 , a 2 = b 2 , b 1 = 2 and use the values of Case 4 into equation (15), we find:

    (34) u 7 ( x , t ) = 4 + sech 2 2 x + 2 t α Γ ( 1 + α ) csch 2 2 x + 2 t α Γ ( 1 + α ) ,

    (35) u 8 ( x , t ) = 4 + sech 2 2 x + 2 t α Γ ( 1 + α ) csch 2 2 x + 2 t α Γ ( 1 + α ) ,

    (36) v 7 ( x , t ) = 4 2 tanh x + 4 t α Γ ( 1 + α ) 2 tanh x + 4 t α Γ ( 1 + α ) ,

    (37) v 8 ( x , t ) = 4 2 coth x + 4 t α Γ ( 1 + α ) 2 coth x + 4 t α Γ ( 1 + α ) ,

    (38) w 7 ( x , t ) = 32 16 tanh x + 4 t α Γ ( 1 + α ) 16 tanh x + 4 t α Γ ( 1 + α ) ,

    (39) w 8 ( x , t ) = 32 16 coth x + 4 t α Γ ( 1 + α ) 16 coth x + 4 t α Γ ( 1 + α ) .

  • Case 5: Let λ = 2 , a 0 = b 2 , a 1 = 0 , a 2 = b 2 , b 1 = ± 2 with b 2 being a free parameter and plug the values of Case 5 into equation (15), we obtain:

(40) u 9 ( x , t ) = tanh 2 2 x + 2 t α Γ ( 1 + α ) coth 2 2 x + 2 t α Γ ( 1 + α ) ,

(41) u 10 ( x , t ) = coth 2 2 x + 2 t α Γ ( 1 + α ) tanh 2 2 x + 2 t α Γ ( 1 + α ) ,

(42) v 9 ( x , t ) = 2 ± 2 1 tanh x 2 t α Γ ( 1 + α ) tanh x 2 t α Γ ( 1 + α ) ,

(43) v 10 ( x , t ) = 2 ± 2 1 coth x 2 t α Γ ( 1 + α ) coth x 2 t α Γ ( 1 + α ) ,

(44) w 9 ( x , t ) = 8 4 2 tanh x 2 t α Γ ( 1 + α ) ¯ tanh x 2 t α Γ ( 1 + α )

(45) w 10 ( x , t ) = 8 4 2 ( coth x 2 t α Γ ( 1 + α ) coth x 2 t α Γ ( 1 + α ) ) .

A picture is an indispensable tool for conversation and to demonstrate the results to the difficulties lucidly. When performing the computation in daily life, we require the fundamental understanding of constructing the use of pictures. Therefore, the graphical presentations of few obtained results are depicted in Figures 1–6.

Figure 1 
               The picture of the result in 
                     
                        
                        
                           
                              
                                 u
                              
                              
                                 1
                              
                           
                           (
                           x
                           ,
                           t
                           )
                        
                        {u}_{1}(x,t)
                     
                   with the values 
                     
                        
                        
                           α
                           =
                           0.35
                        
                        \alpha =0.35
                     
                  , 
                     
                        
                        
                           
                              
                                 b
                              
                              
                                 2
                              
                           
                           =
                           0.5
                        
                        {b}_{2}=0.5
                     
                   and 
                     
                        
                        
                           t
                           =
                           0.01
                        
                        t=0.01
                     
                   for 
                     
                        
                        
                           2
                           D
                        
                        2\text{D}
                     
                   graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.
Figure 1

The picture of the result in u 1 ( x , t ) with the values α = 0.35 , b 2 = 0.5 and t = 0.01 for 2 D graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.

Figure 2 
               The picture of the result in 
                     
                        
                        
                           
                              
                                 u
                              
                              
                                 2
                              
                           
                           (
                           x
                           ,
                           t
                           )
                        
                        {u}_{2}(x,t)
                     
                   with the values 
                     
                        
                        
                           α
                           =
                           0.35
                        
                        \alpha =0.35
                     
                  , 
                     
                        
                        
                           
                              
                                 b
                              
                              
                                 2
                              
                           
                           =
                           0.5
                        
                        {b}_{2}=0.5
                     
                   and 
                     
                        
                        
                           t
                           =
                           0.01
                        
                        t=0.01
                     
                   for 
                     
                        
                        
                           2
                           D
                        
                        2\text{D}
                     
                   graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.
Figure 2

The picture of the result in u 2 ( x , t ) with the values α = 0.35 , b 2 = 0.5 and t = 0.01 for 2 D graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.

Figure 3 
               The picture of the result in 
                     
                        
                        
                           
                              
                                 v
                              
                              
                                 1
                              
                           
                           (
                           x
                           ,
                           t
                           )
                        
                        {v}_{1}(x,t)
                     
                   with the values 
                     
                        
                        
                           α
                           =
                           0.35
                        
                        \alpha =0.35
                     
                  , 
                     
                        
                        
                           
                              
                                 b
                              
                              
                                 2
                              
                           
                           =
                           0.5
                        
                        {b}_{2}=0.5
                     
                   and 
                     
                        
                        
                           t
                           =
                           0.01
                        
                        t=0.01
                     
                   for 
                     
                        
                        
                           2
                           D
                        
                        2\text{D}
                     
                   graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.
Figure 3

The picture of the result in v 1 ( x , t ) with the values α = 0.35 , b 2 = 0.5 and t = 0.01 for 2 D graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.

Figure 4 
               The picture of the result in 
                     
                        
                        
                           
                              
                                 v
                              
                              
                                 2
                              
                           
                           (
                           x
                           ,
                           t
                           )
                        
                        {v}_{2}(x,t)
                     
                   with the unknown parameter values 
                     
                        
                        
                           α
                           =
                           0.35
                        
                        \alpha =0.35
                     
                  , 
                     
                        
                        
                           
                              
                                 b
                              
                              
                                 2
                              
                           
                           =
                           0.5
                        
                        {b}_{2}=0.5
                     
                   and 
                     
                        
                        
                           t
                           =
                           0.01
                        
                        t=0.01
                     
                   for 
                     
                        
                        
                           2
                           D
                        
                        2\text{D}
                     
                   graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.
Figure 4

The picture of the result in v 2 ( x , t ) with the unknown parameter values α = 0.35 , b 2 = 0.5 and t = 0.01 for 2 D graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.

Figure 5 
               The picture of the result in 
                     
                        
                        
                           
                              
                                 v
                              
                              
                                 6
                              
                           
                           (
                           x
                           ,
                           t
                           )
                        
                        {v}_{6}(x,t)
                     
                   with the unknown parameter values 
                     
                        
                        
                           α
                           =
                           0.35
                        
                        \alpha =0.35
                     
                   and 
                     
                        
                        
                           
                              
                                 b
                              
                              
                                 2
                              
                           
                           =
                           0.5
                        
                        {b}_{2}=0.5
                     
                   and 
                     
                        
                        
                           t
                           =
                           0.01
                        
                        t=0.01
                     
                   for 
                     
                        
                        
                           2
                           D
                        
                        2\text{D}
                     
                   graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.
Figure 5

The picture of the result in v 6 ( x , t ) with the unknown parameter values α = 0.35 and b 2 = 0.5 and t = 0.01 for 2 D graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.

Figure 6 
               The picture of the result in 
                     
                        
                        
                           
                              
                                 v
                              
                              
                                 10
                              
                           
                           (
                           x
                           ,
                           t
                           )
                        
                        {v}_{10}(x,t)
                     
                   with the unknown parameter values 
                     
                        
                        
                           α
                           =
                           0.35
                        
                        \alpha =0.35
                     
                  , 
                     
                        
                        
                           
                              
                                 b
                              
                              
                                 2
                              
                           
                           =
                           0.5
                        
                        {b}_{2}=0.5
                     
                   and 
                     
                        
                        
                           t
                           =
                           0.01
                        
                        t=0.01
                     
                   for 
                     
                        
                        
                           2
                           D
                        
                        2\text{D}
                     
                   graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.
Figure 6

The picture of the result in v 10 ( x , t ) with the unknown parameter values α = 0.35 , b 2 = 0.5 and t = 0.01 for 2 D graphics. (a) Real 3D surface, (b) complex 3D surface, (c) 2D shape, (d) real contour shape, (e) complex contour shape.

5 Discussions and future work

In this research, the suggested method has been triumphantly displayed to attain new closed-form wave solutions of equation (13). It has been determined that the complex fractional transformation and the advanced method are an essential and significant mathematical device in analyzing closed-form wave structures of a whole class of fractional FDEs. Consequently, a few new closed-form wave answers of the equation are determined.

The compensations and legality of the recommended approach over the extended Kudryashov approach are as follows. The critical compensation of the proposed method over the extended Kudryashov approach is that the proposed method implements numerous general and plentiful new closed-form wave structures. The closed-form wave solutions of nonlinear FDE have its vital importance to show the complicated physical aspects. For example, [36] extends the Kudryashov method to solve equation Q ξ ( ξ ) = Q 3 ( ξ ) Q ( ξ ) as an auxiliary equation and the closed-form solutions presented by u ( ξ ) = i = 0 n α i Q i ( ξ ) , where Q ( ξ ) = ± 1 1 ± e 2 ξ . Our solutions u 1 , v 1 , w 1 , u 2 , v 2 , w 2 , u 5 and u 6 are similar to solutions of [36] and solutions u 3 , v 3 , w 3 , u 4 , v 4 , w 4 , v 5 , w 5 , v 6 , w 6 , u 7 , v 7 , w 7 , u 8 , v 8 , w 8 , u 9 , v 9 , w 9 , u 10 , v 10 and w 10 are all new exact solutions obtained in this paper, which validates our proposed methods. Although we have presented diverse closed-form wave solutions by performing the recommended method, our obtained solutions show that our proposed methods are more helpful and extraordinary in contributing much more general and many new closed-form wave solutions at the same time. To state the effectiveness and present the insight of processes and the comparison among our proposed method, the new ansatz method is much more proficient than the new extended Kudryashov method. We can underline from our understanding that the method can be performed in other nonlinear FDEs and can reduce the amount of computational work. Therefore, the investigation of closed-form wave structures of other nonlinear FDEs deserves further analysis.

Acknowledgements

The authors would like to acknowledge CAS-TWAS president’s fellowship program. The author thanks the referees for their suggestions and comments.

  1. Competing interests: This research received no specific grant from any funding agency in the public, commercial or not-for-profit sectors. The authors did not have any competing interests in this research.

  2. Author contributions: All parts contained in the research carried out by the authors through hard work and a review of the various references and contributions in the field of mathematics and Applied physics.

  3. Availability of data and materials: Data sharing is not applicable to this article as no datasets were generated or analyzed during the current study.

  4. Funding: No funding for this article.

References

[1] Podlubny I . Fractional Differential Equations. New York: Academic Press; 1999.Search in Google Scholar

[2] Miller KS , Ross B . An Introduction to the Fractional Calculus and Fractional Differential Equations. New York: John Wiley; 1993.Search in Google Scholar

[3] Mainardi F . Fractional Calculus Some Basic Problems in Continum and Statistical Mechanics. New York: Springer-Verlag; 1997.10.1007/978-3-7091-2664-6Search in Google Scholar

[4] Alam M , Belgacem F . Microtubules nonlinear models dynamics investigations through the exp(−ϕ(ξ))-expansion method implementation. Mathematics. 2016;4:6.10.3390/math4010006Search in Google Scholar

[5] Alam M , Tunc C . An analytical method for solving exact solutions of the nonlinear bogoyavlenskii equation and the nonlinear diffusive predator-prey system. Alex Eng J. 2016;55:1855–65.10.1016/j.aej.2016.04.024Search in Google Scholar

[6] Sonmezoglu A . Exact solutions for some fractional differential equations. Adv Math Phys. 2015;2015:567842 10.1155/2015/567842Search in Google Scholar

[7] Karaagac B . New exact solutions for some fractional order differential equations via improved sub-equation method. Discret Cont Dyn Syst – S. 2019;12:447–54.10.3934/dcdss.2019029Search in Google Scholar

[8] Iqbal M , Seadawy AR , Lu D . Construction of solitary wave solutions to the nonlinear modified Kortewege-de Vries dynamical equation in unmagnetized plasma via mathematical methods. Mod Phys Lett A. 2018;33(32):1850183.10.1142/S0217732318501833Search in Google Scholar

[9] Martineza HY , Aguilarb JFG , Baleanu D . Beta-derivative and sub-equation method applied to the optical solitons in medium with parabolic law nonlinearity and higher order dispersion. Optik. 2018;155:357–65.10.1016/j.ijleo.2017.10.104Search in Google Scholar

[10] Saleh R , Kassem M , Mabrouk SM . Exact solutions of nonlinear fractional order partial differential equations via singular manifold method. Chin J Phys. 2019;61:290–300.10.1016/j.cjph.2019.09.005Search in Google Scholar

[11] Delgado VFM , Aguilar JFG , Torres L , Jimenez RFE , Hernandez MAT . Exact solutions for the liénard type model via fractional homotopy methods. Fract Derivatives Mittag–Leffler Kernel. 2019;194:269–91.10.1007/978-3-030-11662-0_16Search in Google Scholar

[12] Abuasad S , Moaddy K , Hashim I . Analytical treatment of two-dimensional fractional helmholtz equations. J King Saud Univ – Sci. 2019;31:659–66.10.1016/j.jksus.2018.02.002Search in Google Scholar

[13] Alam MN , Tunc C . Constructions of the optical solitons and others soliton to the conformable fractional zakharov–kuznetsov equation with power law nonlinearity. J Taibah Univ Med Sci. 2020;15:263–72. 10.1080/16583655.2019.1708542.Search in Google Scholar

[14] Seadawy AR . Three-dimensional weakly nonlinear shallow water waves regime and its travelling wave solutions. Int J Comput Methods. 2018;15:1850017.10.1142/S0219876218500172Search in Google Scholar

[15] Kadkhoda N , Jafari H . An analytical approach to obtain exact solutions of some space-time conformable fractional differential equations. Adv Differ Equ. 2019;2019;428.10.1186/s13662-019-2349-0Search in Google Scholar

[16] Seadawy AR , Manafian J . New soliton solution to the longitudinal wave equation in a magneto-electro-elastic circular rod. Results Phys. 2018;8:1158–67.10.1016/j.rinp.2018.01.062Search in Google Scholar

[17] Lu D , Seadawy AR , Ali A . Dispersive traveling wave solutions of the equal-width and modified equal-width equations via mathematical methods and its applications. Results Phys. 2018;9:313–20.10.1016/j.rinp.2018.02.036Search in Google Scholar

[18] Helal MA , Seadawy AR , Zekry MH . Stability analysis of solitary wave solutions for the fourth-order nonlinear Boussinesq water wave equation. Appl Math Comput. 2014;232:1094–103.10.1016/j.amc.2014.01.066Search in Google Scholar

[19] Shi D , Zhang Y . Diversity of exact solutions to the conformable space-time fractional mew equation. Appl Math Lett. 2020;99:105994.10.1016/j.aml.2019.07.025Search in Google Scholar

[20] Seadawy AR , El-Rashidy K . Dispersive solitary wave solutions of kadomtsev–petviashivili and modified kadomtsev–petviashivili dynamical equations in unmagnetized dust plasma. Results Phys. 2018;8:1216–22.10.1016/j.rinp.2018.01.053Search in Google Scholar

[21] Lu D , Seadawy AR , Ali A . Applications of exact traveling wave solutions of modified Liouville and the symmetric regularized long wave equations via two new techniques. Results Phys. 2018;9:1403–10.10.1016/j.rinp.2018.04.039Search in Google Scholar

[22] Arshad M , Seadawy A , Lu D . Elliptic function and solitary wave solutions of the higher-order nonlinear Schrodinger dynamical equation with fourth-order dispersion and cubic-quintic nonlinearity and its stability. Eur Phys J Plus. 2017;132:371.10.1140/epjp/i2017-11655-9Search in Google Scholar

[23] Zuriqat M . Exact solution for the fractional partial differential equation by homo separation analysis method. Afr Matematika. 2019;30:1133–43.10.1007/s13370-019-00707-xSearch in Google Scholar

[24] Arnous AH , Seadawy AR , Alqahtani RT , Biswas A . Optical solitons with complex ginzburg-landau equation by modified simple equation method. Opt – Int J Light Electron Opt. 2017;144:475–80.10.1016/j.ijleo.2017.07.013Search in Google Scholar

[25] Owyed S , Abdou MA , Abdel-Atyb AH , Nekhili WAR . Numerical and approximate solutions for coupled time fractional nonlinear evolutions equations via reduced differential transform method. Chaos, Solitons Fractals. 2019;217:109474.10.1016/j.chaos.2019.109474Search in Google Scholar

[26] Abdullah , Seadawy AR , Wang J . Mathematical methods and solitary wave solutions of three-dimensional zakharov–kuznetsov–burgers equation in dusty plasma and its applications. Results Phys. 2017;7:4269–77.10.1016/j.rinp.2017.10.045Search in Google Scholar

[27] Cenesiz Y , Tasbozan O , Kurt A . Functional variable method for conformable fractional modified kdv-zkequation and maccari system. Tbilisi Math J. 2017;10:117–25.10.1515/tmj-2017-0010Search in Google Scholar

[28] Seadawy AR , Lu D , Yue C . Travelling wave solutions of the generalized nonlinear fifth-order kdv water wave equations and its stability. J Taibah Univ Sci. 2017;11:623–33.10.1016/j.jtusci.2016.06.002Search in Google Scholar

[29] Sheikholeslami M . Cuo-water nanofluid free convection in a porous cavity considering darcy law. Eur Phys J Plus. 2017;132:132.10.1140/epjp/i2017-11330-3Search in Google Scholar

[30] Khater AH , Callebaut DK , Seadawy AR . General soliton solutions for nonlinear dispersive waves in convective type instabilities. Phys Scr. 2006;74:384–93.10.1088/0031-8949/74/3/015Search in Google Scholar

[31] Shehata AR , Abu-Amra SSM . Geometrical properties and exact solutions of three (3 + 1) -dimensional nonlinear evolution equations in mathematical physics using different expansion methods. J Adv Math Comput Sci. 2019;33:1–19.10.9734/jamcs/2019/v32i430149Search in Google Scholar

[32] Unal E , Gokdogan A . Solution of conformable fractional ordinary differential equations via differential transform method. Opt – Int J Light Electron Opt. 2017;128:264–73.10.1016/j.ijleo.2016.10.031Search in Google Scholar

[33] Alam MN , Li X . Exact traveling wave solutions to higher order nonlinear equations. J Ocean Eng Sci. 2019;4:276–88.10.1016/j.joes.2019.05.003Search in Google Scholar

[34] Arshad M , Seadawy A , Lu D . Modulation stability and optical soliton solutions of nonlinear Schrodinger equation with higher order dispersion and nonlinear terms and its applications. Superlattices Microstructures. 2017;112:422–34.10.1016/j.spmi.2017.09.054Search in Google Scholar

[35] Eslami M . Exact traveling wave solutions to the fractional coupled nonlinear schrodinger equations. Appl Math Comput. 2016;285:141–8.10.1016/j.amc.2016.03.032Search in Google Scholar

[36] Ege S , Misirli E . A new method for solving nonlinear fractional differential equations. N Trends Math Sci. 2017;5:225–33.10.20852/ntmsci.2017.141Search in Google Scholar

[37] Wazwaz A . Exact solutions with solitons and periodic structures for the zakharov–kuznetsov equation and its modified form. Commun Nonlinear Sci Numer Simul. 2005;10:597–606.10.1016/j.cnsns.2004.03.001Search in Google Scholar

[38] Akbulut MKA , Bekir A . Auxiliary equation method for fractional differential equations with modified riemann–liouville derivative. Int J Nonlin Sci Num. 2016;17:413–20.10.1515/ijnsns-2016-0023Search in Google Scholar

[39] Aly Seadawy , El-Rashidy K . Dispersive solitary wave solutions of Kadomtsev–Petviashivili and modified Kadomtsev–Petviashivili dynamical equations in unmagnetized dust plasma. Results Phys. 2018;8:1216–22.10.1016/j.rinp.2018.01.053Search in Google Scholar

[40] Kumar S , Kumar R , Singh J , Nisar KS , Kumard D . An efficient numerical scheme for fractional model of HIV-1 infection of CD4 + T-cells with the effect of antiviral drug therapy. Alex Eng J. 2020;216:634–42. 10.1016/j.aej.2019.12.046 Search in Google Scholar

[41] Kumar S , Kumar A , Momani S , Aldhaifallah M , Nisar KS . Numerical solutions of nonlinear fractional model arising in the appearance of the stripe patterns in two-dimensional systems. Adv Differ Equ. 2019;2019(1):413.10.1186/s13662-019-2334-7Search in Google Scholar

[42] Kumar S , Kumar A , Abbas S , Qurashi MA , Baleanu D . A modified analytical approach with existence and uniqueness for fractional Cauchy reaction-diffusion equations. Adv Differ Equ. 2020;2020(1):1–8.10.1186/s13662-019-2488-3Search in Google Scholar

[43] Sharma B , Kumar S , Cattani C , Baleanu D . Nonlinear dynamics of Cattaneo–Christov heat flux model for third-grade power-law fluid. J Comput Nonlinear Dyn. 2020 Jan 1;15(1):927–41.10.1115/1.4045406Search in Google Scholar

[44] Kumar S , Ghosh S , Samet B , Goufo EFD . An analysis for heat equations arises in diffusion process using new Yang–AbdelAty–Cattani fractional operator. Math Methods Appl Sci. 2020;162:572–84.Search in Google Scholar

[45] Tassaddiq A , Khan I , Nisar KS . Heat transfer analysis in sodium alginate based nanofluid using MoS2 nanoparticles: Atangana–Baleanu fractional model. Chaos, Solitons Fractals. 2020;130:109445.10.1016/j.chaos.2019.109445Search in Google Scholar

[46] Gao W , Senel M , Yel G , Baskonus HM , Senel B . New complex wave patterns to the electrical transmission line model arising in network system. Aims Math. 2020;5(3):1881–92.10.3934/math.2020125Search in Google Scholar

[47] Gao W , Ismael HF , Husien AM , Bulut H , Baskonus HM . Optical soliton solutions of the nonlinear Schrödinger and resonant nonlinear Schrödinger equation with Parabolic law. Appl Sci. 2020;10(1):219 , 1–20.10.3390/app10010219Search in Google Scholar

[48] Gao W , Yel G , Baskonus HM , Cattani C . Complex solitons in the conformable (2 + 1)-dimensional Ablowitz–Kaup–Newell–Segur equation. Aims Math. 2020;5(1):507–21.10.3934/math.2020034Search in Google Scholar

[49] Gao W , Rezazadeh H , Pinar Z , Baskonus HM , Sarwar S , Yel G . Novel explicit solutions for the nonlinear zoomeron equation by using newly extended direct algebraic technique. Opt Quant Electron. 2020;52(52):1–13.10.1007/s11082-019-2162-8Search in Google Scholar

[50] Cordero A , Jaiswal JP , Torregrosa JR . Stability analysis of fourth-order iterative method for finding multiple roots of non-linear equations. Appl Math Nonlinear Sci. 2019;4(1):43–56.10.2478/AMNS.2019.1.00005Search in Google Scholar

[51] Jumarie G . Table of some basic fractional calculus formulae derived from a modified riemann–liouville derivative for non-differentiable functions. Appl Math Lett. 2009;22:378–85.10.1016/j.aml.2008.06.003Search in Google Scholar

[52] Guner O . Singular and non-topological soliton solutions for nonlinear fractional differential equations. Chin Phys B. 2015;24:100201.10.1088/1674-1056/24/10/100201Search in Google Scholar

[53] Hartley T , Lorenzo C . Dynamics and control of initialized fractional-order systems. Nonlinear Dyn. 2002;29:201–33.10.1023/A:1016534921583Search in Google Scholar

[54] Kilbas A , Srivastava H , Trujillo J . Theory and applications of fractional differential equations. Amsterdam: Elsevier; 2006.Search in Google Scholar

Received: 2020-05-27
Revised: 2020-07-29
Accepted: 2020-07-29
Published Online: 2020-09-24

© 2020 Md Nur Alam et al., published by De Gruyter

This work is licensed under the Creative Commons Attribution 4.0 International License.

Articles in the same Issue

  1. Regular Articles
  2. Model of electric charge distribution in the trap of a close-contact TENG system
  3. Dynamics of Online Collective Attention as Hawkes Self-exciting Process
  4. Enhanced Entanglement in Hybrid Cavity Mediated by a Two-way Coupled Quantum Dot
  5. The nonlinear integro-differential Ito dynamical equation via three modified mathematical methods and its analytical solutions
  6. Diagnostic model of low visibility events based on C4.5 algorithm
  7. Electronic temperature characteristics of laser-induced Fe plasma in fruits
  8. Comparative study of heat transfer enhancement on liquid-vapor separation plate condenser
  9. Characterization of the effects of a plasma injector driven by AC dielectric barrier discharge on ethylene-air diffusion flame structure
  10. Impact of double-diffusive convection and motile gyrotactic microorganisms on magnetohydrodynamics bioconvection tangent hyperbolic nanofluid
  11. Dependence of the crossover zone on the regularization method in the two-flavor Nambu–Jona-Lasinio model
  12. Novel numerical analysis for nonlinear advection–reaction–diffusion systems
  13. Heuristic decision of planned shop visit products based on similar reasoning method: From the perspective of organizational quality-specific immune
  14. Two-dimensional flow field distribution characteristics of flocking drainage pipes in tunnel
  15. Dynamic triaxial constitutive model for rock subjected to initial stress
  16. Automatic target recognition method for multitemporal remote sensing image
  17. Gaussons: optical solitons with log-law nonlinearity by Laplace–Adomian decomposition method
  18. Adaptive magnetic suspension anti-rolling device based on frequency modulation
  19. Dynamic response characteristics of 93W alloy with a spherical structure
  20. The heuristic model of energy propagation in free space, based on the detection of a current induced in a conductor inside a continuously covered conducting enclosure by an external radio frequency source
  21. Microchannel filter for air purification
  22. An explicit representation for the axisymmetric solutions of the free Maxwell equations
  23. Floquet analysis of linear dynamic RLC circuits
  24. Subpixel matching method for remote sensing image of ground features based on geographic information
  25. K-band luminosity–density relation at fixed parameters or for different galaxy families
  26. Effect of forward expansion angle on film cooling characteristics of shaped holes
  27. Analysis of the overvoltage cooperative control strategy for the small hydropower distribution network
  28. Stable walking of biped robot based on center of mass trajectory control
  29. Modeling and simulation of dynamic recrystallization behavior for Q890 steel plate based on plane strain compression tests
  30. Edge effect of multi-degree-of-freedom oscillatory actuator driven by vector control
  31. The effect of guide vane type on performance of multistage energy recovery hydraulic turbine (MERHT)
  32. Development of a generic framework for lumped parameter modeling
  33. Optimal control for generating excited state expansion in ring potential
  34. The phase inversion mechanism of the pH-sensitive reversible invert emulsion from w/o to o/w
  35. 3D bending simulation and mechanical properties of the OLED bending area
  36. Resonance overvoltage control algorithms in long cable frequency conversion drive based on discrete mathematics
  37. The measure of irregularities of nanosheets
  38. The predicted load balancing algorithm based on the dynamic exponential smoothing
  39. Influence of different seismic motion input modes on the performance of isolated structures with different seismic measures
  40. A comparative study of cohesive zone models for predicting delamination fracture behaviors of arterial wall
  41. Analysis on dynamic feature of cross arm light weighting for photovoltaic panel cleaning device in power station based on power correlation
  42. Some probability effects in the classical context
  43. Thermosoluted Marangoni convective flow towards a permeable Riga surface
  44. Simultaneous measurement of ionizing radiation and heart rate using a smartphone camera
  45. On the relations between some well-known methods and the projective Riccati equations
  46. Application of energy dissipation and damping structure in the reinforcement of shear wall in concrete engineering
  47. On-line detection algorithm of ore grade change in grinding grading system
  48. Testing algorithm for heat transfer performance of nanofluid-filled heat pipe based on neural network
  49. New optical solitons of conformable resonant nonlinear Schrödinger’s equation
  50. Numerical investigations of a new singular second-order nonlinear coupled functional Lane–Emden model
  51. Circularly symmetric algorithm for UWB RF signal receiving channel based on noise cancellation
  52. CH4 dissociation on the Pd/Cu(111) surface alloy: A DFT study
  53. On some novel exact solutions to the time fractional (2 + 1) dimensional Konopelchenko–Dubrovsky system arising in physical science
  54. An optimal system of group-invariant solutions and conserved quantities of a nonlinear fifth-order integrable equation
  55. Mining reasonable distance of horizontal concave slope based on variable scale chaotic algorithms
  56. Mathematical models for information classification and recognition of multi-target optical remote sensing images
  57. Hopkinson rod test results and constitutive description of TRIP780 steel resistance spot welding material
  58. Computational exploration for radiative flow of Sutterby nanofluid with variable temperature-dependent thermal conductivity and diffusion coefficient
  59. Analytical solution of one-dimensional Pennes’ bioheat equation
  60. MHD squeezed Darcy–Forchheimer nanofluid flow between two h–distance apart horizontal plates
  61. Analysis of irregularity measures of zigzag, rhombic, and honeycomb benzenoid systems
  62. A clustering algorithm based on nonuniform partition for WSNs
  63. An extension of Gronwall inequality in the theory of bodies with voids
  64. Rheological properties of oil–water Pickering emulsion stabilized by Fe3O4 solid nanoparticles
  65. Review Article
  66. Sine Topp-Leone-G family of distributions: Theory and applications
  67. Review of research, development and application of photovoltaic/thermal water systems
  68. Special Issue on Fundamental Physics of Thermal Transports and Energy Conversions
  69. Numerical analysis of sulfur dioxide absorption in water droplets
  70. Special Issue on Transport phenomena and thermal analysis in micro/nano-scale structure surfaces - Part I
  71. Random pore structure and REV scale flow analysis of engine particulate filter based on LBM
  72. Prediction of capillary suction in porous media based on micro-CT technology and B–C model
  73. Energy equilibrium analysis in the effervescent atomization
  74. Experimental investigation on steam/nitrogen condensation characteristics inside horizontal enhanced condensation channels
  75. Experimental analysis and ANN prediction on performances of finned oval-tube heat exchanger under different air inlet angles with limited experimental data
  76. Investigation on thermal-hydraulic performance prediction of a new parallel-flow shell and tube heat exchanger with different surrogate models
  77. Comparative study of the thermal performance of four different parallel flow shell and tube heat exchangers with different performance indicators
  78. Optimization of SCR inflow uniformity based on CFD simulation
  79. Kinetics and thermodynamics of SO2 adsorption on metal-loaded multiwalled carbon nanotubes
  80. Effect of the inner-surface baffles on the tangential acoustic mode in the cylindrical combustor
  81. Special Issue on Future challenges of advanced computational modeling on nonlinear physical phenomena - Part I
  82. Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications
  83. Some new extensions for fractional integral operator having exponential in the kernel and their applications in physical systems
  84. Exact optical solitons of the perturbed nonlinear Schrödinger–Hirota equation with Kerr law nonlinearity in nonlinear fiber optics
  85. Analytical mathematical schemes: Circular rod grounded via transverse Poisson’s effect and extensive wave propagation on the surface of water
  86. Closed-form wave structures of the space-time fractional Hirota–Satsuma coupled KdV equation with nonlinear physical phenomena
  87. Some misinterpretations and lack of understanding in differential operators with no singular kernels
  88. Stable solutions to the nonlinear RLC transmission line equation and the Sinh–Poisson equation arising in mathematical physics
  89. Calculation of focal values for first-order non-autonomous equation with algebraic and trigonometric coefficients
  90. Influence of interfacial electrokinetic on MHD radiative nanofluid flow in a permeable microchannel with Brownian motion and thermophoresis effects
  91. Standard routine techniques of modeling of tick-borne encephalitis
  92. Fractional residual power series method for the analytical and approximate studies of fractional physical phenomena
  93. Exact solutions of space–time fractional KdV–MKdV equation and Konopelchenko–Dubrovsky equation
  94. Approximate analytical fractional view of convection–diffusion equations
  95. Heat and mass transport investigation in radiative and chemically reacting fluid over a differentially heated surface and internal heating
  96. On solitary wave solutions of a peptide group system with higher order saturable nonlinearity
  97. Extension of optimal homotopy asymptotic method with use of Daftardar–Jeffery polynomials to Hirota–Satsuma coupled system of Korteweg–de Vries equations
  98. Unsteady nano-bioconvective channel flow with effect of nth order chemical reaction
  99. On the flow of MHD generalized maxwell fluid via porous rectangular duct
  100. Study on the applications of two analytical methods for the construction of traveling wave solutions of the modified equal width equation
  101. Numerical solution of two-term time-fractional PDE models arising in mathematical physics using local meshless method
  102. A powerful numerical technique for treating twelfth-order boundary value problems
  103. Fundamental solutions for the long–short-wave interaction system
  104. Role of fractal-fractional operators in modeling of rubella epidemic with optimized orders
  105. Exact solutions of the Laplace fractional boundary value problems via natural decomposition method
  106. Special Issue on 19th International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering
  107. Joint use of eddy current imaging and fuzzy similarities to assess the integrity of steel plates
  108. Uncertainty quantification in the design of wireless power transfer systems
  109. Influence of unequal stator tooth width on the performance of outer-rotor permanent magnet machines
  110. New elements within finite element modeling of magnetostriction phenomenon in BLDC motor
  111. Evaluation of localized heat transfer coefficient for induction heating apparatus by thermal fluid analysis based on the HSMAC method
  112. Experimental set up for magnetomechanical measurements with a closed flux path sample
  113. Influence of the earth connections of the PWM drive on the voltage constraints endured by the motor insulation
  114. High temperature machine: Characterization of materials for the electrical insulation
  115. Architecture choices for high-temperature synchronous machines
  116. Analytical study of air-gap surface force – application to electrical machines
  117. High-power density induction machines with increased windings temperature
  118. Influence of modern magnetic and insulation materials on dimensions and losses of large induction machines
  119. New emotional model environment for navigation in a virtual reality
  120. Performance comparison of axial-flux switched reluctance machines with non-oriented and grain-oriented electrical steel rotors
  121. Erratum
  122. Erratum to “Conserved vectors with conformable derivative for certain systems of partial differential equations with physical applications”
Downloaded on 13.9.2025 from https://www.degruyterbrill.com/document/doi/10.1515/phys-2020-0179/html
Scroll to top button