Application of double Sumudu-generalized Laplace decomposition method and two-dimensional time-fractional coupled Burger’s equation

The current paper concentrates on discovering the exact solutions of the time-fractional regular and singular coupled Burger’s equations by involving a new technique known as the double Sumudu-generalized Laplace and Adomian decomposition method. Furthermore, some theorems of the double Sumudu-generalized Laplace properties are proved. Further, the oﬀered method is a powerful tool for solving an enormous number of problems. The precision of the technique is evaluated with the aid of some examples, this method oﬀers a solution precisely and successfully in a series form with smoothly calculated coeﬃcients. The relation between both the approximate and exact solution is represented by a graph to display the high speed of this method’s convergence.


Introduction
Burger's equation is one of the fundamental and essential nonlinear partial differential equations (PDE) containing diffusive properties and nonlinear expansion effects.Burger's equation was improved as a model of disorderly fluid movement.The fractional Burger's equation has received much interest and the solution to this problem becomes essential for mathematicians and physical phenomena.This problem has been found to demonstrate various types of events, for instance, a mathematical model of turbulence and an approximate theorem of flow through a trauma wave traveling in a viscous liquid [1,2].The authors in [3] introduced a semianalytical method that is called the local fractional Laplace homotopy analysis method to solve wave equations with local fractional derivatives and the authors used the same method to solve differential equations involving local fractional derivatives based on the local fractional calculus [4].The Shehu transform and a semianalytical method have been used to solve multidimensional fractional diffusion equations [5].The numerical solution of three-dimensional coupled Burger's Equations has been studied by the Laplace decomposition method in [6,7].In recent years, substantial confirmation was offered on the Laplace decomposition method and its changes for discussing mathematical problems [8,9].In a previous study, the authors recommended various kinds of approximation and exact technique to solve fractional Burger's equation methods [10][11][12].The researchers in [13] suggested the variational iteration method to gain Burger's equation.In [14], the Laplace decomposition method (LDM) was applied to determine the solution of two-dimensional nonlinear Burger's equations.The authors in [15] proposed a modification of the double Laplace decomposition method to obtain an analytical approximation solution of a coupled system of Burger's equation.There are many approaches where one can obtain a series of solutions, such as the Modified Laplace variational iteration method [16], and the He-Laplace method [17].The approximate solution of wave problems in multidimensional orders was studied by applying the Aboodh homotopy integral transform method (AHITM), see [18].The authors in [19] used the Yang Transform to obtain the approximation solution of nonlinear time-fractional Klein-Gordon equations.The authors in [20] employed the Fountain theorem and the symmetric Mountain-Pass theorem to study the novel trinonlocal Kirchhoff problem.The main aim of this paper is to offer a new hybrid of a double Sumudu-Generalized Laplace Transform to determine the exact solutions of the time-fractional regular and singular coupled Burger's equations.Finally, examples are given to clarify the proposed technique.Definitions will be recalled; the double Sumudu transform and the Generalized Laplace Transform that are useful in this article.
Definition 1 [21] let ψ(χ, σ ) be a function we define as the double Sumudu Transform of function ψ(χ, σ ), σ , χ ∈ R + is given by The generalized Laplace transform of the function ψ(t) is given by G α in the following definition.
Definition 2 If ψ(t) is an integrable function defined for all t ≥ 0, its generalized Laplace transform G α is the integral of ψ(t) times s α e -t s from t = 0 to ∞.It is a function of s, say (s), and is denoted by G α (ψ); thus where, s ∈ C and α ∈ Z, for more details see [22].

Main results of double Sumudu-generalized Laplace transform
The definitions and existence condition of the double Sumudu-generalized Laplace transform are presented in this section.Here, we work with the double Sumudu-generalized Laplace transform, which is defined by and we note that the double Sumudu-generalized Laplace transform is a hybrid between the double Sumudu transform and the generalized Laplace transform.From the definition of the double Sumudu-generalized Laplace transform, we conclude the following: 1. if we put α = 0 and s = 1 s we obtain the double Sumudu-Laplace transform ( 2 ) 2. if we put α = 0 and replacing s by we obtain the double Sumudu-Yang Transform ( 3 ) 3. At α = -1 and replacing s by μ 3 we obtain the triple Sumudu Transform ) dt dσ dχ; ( 4 ) 4. At α = 1 we obtain the double Sumudu-Elzaki transform ( 5 ) 5. At α = -1 and 1 v = 1 s we obtain the double Sumudu-Aboodh transform From the analysis above concerning the double Sumudu-generalized Laplace transform, we note that the hybrid of the double Sumudu-generalized Laplace transform is more generic than the above transforms.Hence, the double Sumudu-generalized Laplace decomposition method is considered the most generic amongst other related methods.
The double Sumudu-generalized Laplace transform of the function and The next theorem offers the double Sumudu-generalized Laplace transform of the partial derivatives χD β t ψ and σ D β t ψ.

Theorem 3 The double Sumudu-generalized Laplace transform of the fractional partial derivatives
Proof By employing partial derivatives according to μ 1 for Eq. ( 1), we obtain and the partial derivative within the brackets can be calculated as follows: by putting Eq. ( 23) into Eq.( 22), we obtain therefore, Eq. ( 24) becomes hence, and by arranging the above equation, we will obtain the proof of Eq. ( 20) as follows Similarly, we can prove Eq. ( 21).
The double Sumudu-generalized Laplace transform of the partial derivatives is presented in the upcoming theorem: Theorem 4 The double Sumudu-generalized Laplace transform of the fractional partial derivatives χσ D - Proof By taking partial derivatives according to μ 1 for Eq. ( 1), we have and we calculate the partial derivative inside brackets as follows: Putting Eq. (29) into Eq.(28), we obtain the partial derivative with respect to μ 2 for Eq. ( 30) is calculated as the following: therefore, Eq. (31) becomes and one can rearrange Eq. ( 33), to prove Eq. ( 27)

Double Sumudu-generalized Laplace decomposition method and two-dimensional time-fractional coupled Burger's equation
This section aims to make use of the double Sumudu-generalized Laplace decomposition method (DSGLTDM) to solve the two-dimensional time-fractional coupled Burger's equation.In the upcoming analysis, we deem the two-dimensional fractional coupled Burger's equation to be: with the following conditions where D β t = ∂ β ∂t β stands for the fractional Caputo derivative, is the Reynolds number, and the velocity components are determined by ψ(χ, σ , t) and φ(χ, σ , t) in the χ and σ directions, respectively.The two-dimensional coupled Burger's equations are the same as the incompressible Navier-Stokes equations with the pressure-gradient terms removed.With the purpose to gain the solution of Eq. (34), first, operating the double Sumudugeneralized Laplace for Eq.(34) and using the double Sumudu transform for Eq. ( 35) we gain and by putting Eq. ( 19) into Eq.(36) and Eq.(37), we obtain and therefore, by rearranging Eq. (38) and Eq.(39) we obtain and and by employing the inverse double Sumudu-generalized Laplace for Eq.(38) and Eq.(39), we yield and where some terms of the Adomian polynomials A n B n , C n , and D n are determined by and S -1 s denotes the inverse double Sumudu-generalized Laplace.The double Sumudu-generalized Laplace decomposition method (DSGLTDM) defines the solutions ψ(χ, σ , t) and ψ(χ, σ , t) and is represented by the following infinite series.
Moreover, the nonlinear terms ψψ χ , φ ∂ψ ∂σ , ψ ∂φ ∂χ and φ ∂φ ∂σ are presented by: By substituting Eq. ( 48) and Eq.(49) into Eq.( 42) and Eq. ( 43), we obtain and By comparing both sides of Eq. ( 51) and Eq. ( 52), we obtain Generally, the remnant terms are presented by and where the inverse double Sumudu-generalized Laplace transform is determined by We assume that the inverse exists for Eqs.(54) and (55).For the goal of illustrating the advantages and the reliability of the (DSGLTDM) we solve the two-dimensional fractional coupled Burger's equations.
Example 1 [13,26,27] Consider the singular two-dimensional time-fractional coupled Burger's equations to be determined by with the following conditions Utilizing the previous steps one can obtain The zeroth components ψ 0 and φ 0 are proposed by the Adomian method; combining the initial conditions and the sources terms as follows: The remainder components ψ n+1 , φ n+1 , n ≥ 0 are determined by utilizing the relation and for n = 0, 1, 2, . . ., so, at n = 0 and , likely, at n = 1, we have and at n = 2, we produce , similar to .
Thus, the solution of Eq. ( 56) is We achieved the same results that were presented in [13,26,27].The comparison between the exact and numerical solutions for the Eq. ( 56) is shown in Figs. 1 and 2. We obtain the exact solution at β = 1 and the different values of β such as (β = 0.95, β = 0.99) shows the approximate solution.The surfaces in Figs. 3 and 4 show the exact solution of the functions ψ(χ, σ , t) and φ(χ, σ , t) at χ = 0, respectively.

Double Sumudu-generalized Laplace decomposition method and singular two-dimensional time-fractional coupled Burger's equation
The objective of this section is to interpret the utilization of the double Sumudugeneralized Laplace decomposition method for solving the singular two-dimensional time-fractional coupled Burger's equations in the following form with the initial condition where σ (σ φ σ ) σ are the so-called Bessel operators, ψ(χ, σ , t) and φ(χ, σ , t) are the velocity components to be presented, f (χ, σ , t), g(χ, σ , t), f 1 (χ, σ ), and g 1 (χ, σ ) are given functions.For the purpose of obtaining the solution of Eq. ( 62), we apply the next steps: Step 1: Multiply both sides of Eq. ( 62) by χσ to yield Step 2: Taking the double Sumudu-generalized Laplace transform for either side of Eq. (64) we gain and Step 3: By taking the double integral for both sides of Eq. ( 65) and Eq.(66) from 0 to μ 1 and 0 to μ 2 according to μ 1 and μ 2 , respectively, we obtain and Step 4: On using the inverse double Sumudu-generalized Laplace decomposition method for Eqs.(67) and (68), we obtain and Step 5: Substituting Eqs. ( 48), (50), and Eq.(49) into Eqs.( 69) and (70), we have Step 6: On utilizing the double Sumudu-generalized Laplace decomposition method, we present the recursive relations to obtain: and The remainder components ψ n+1 and φ n+1 , n ≥ 0 are determined by and and S χ S σ G t is the double Sumudu-generalized Laplace transform with respect to χ , σ , t and the inverse double Sumudu-generalized Laplace transform is denoted by S -1 μ 1 S -1 μ 2 G -1 s according to μ 1 , μ 2 , s.We assumed that the inverse double Sumudu-generalized Laplace transform with respect to μ 1 , μ 2 , and s exists for Eqs. ( 71), ( 72), (73), and (74).In the following example, we use the double Sumudu-generalized Laplace transform Adomain decomposition method to solve singular two-dimensional time-fractional coupled Burger's equations.
Example 2 [26] Consider that the singular two-dimensional time-fractional coupled Burger's equations are presented by with the initial condition By using our method above, we successfully obtain and the remainder components ψ n+1 and φ n+1 , n ≥ 0 are given by and By substituting n = 0, into Eqs.( 76) and (77) we have In a similar way, at n = 1, we have The solution of Eq. ( 75) is determined by Thence, the exact solution is denoted by when we put α = 1, we obtain the exact solution of Eq. (75) as follows:   The comparison between the exact and numerical solutions for the Eq. ( 75) is shown in Figs. 5 and 6.We obtain the exact solution at β = 1 and the different values of β such as (β = 0.95, β = 0.99) shows the approximate solution.The surfaces in Figs.7 and 8 show the exact solution of the functions ψ(χ, σ , t) and φ(χ, σ , t) at χ = 0, respectively.

Conclusions
In this research paper, double Sumudu-generalized Laplace transforms and Adomian decomposition have been profitably joined to obtain a new potent method called the double Sumudu-generalized Laplace Adomian decomposition method (DSGLTDM).This technique has been employed to solve regular and singular two-dimensional time-fractional coupled Burger's equations.By involving this approach in some examples we have obtained new effective relations to solve our problems.Our method shows that the series solution can converge very quickly to the solutions.In this study, the technique utilized to obtain exact and approximation solutions can also be expanded to solve other nonlinear partial differential equations of physical interest.We see that the results of Examples 1 and 2 are the same as those of applying the Laplace-Adomian decomposition method, vari-Figure 8 The surface shows the function φ(χ, σ , t) ational iteration method (VIM), and Triple Laplace-Adomian Decomposition Method, [13,26,27].The advantage of DSGLTDM is that it generates other methods, such as the double Sumudu-Laplace transform decomposition method, see Eq. ( 2), the double Sumudu-Yang Transform decomposition method, see Eq. ( 3), the triple Sumudu Transform decomposition method, see Eq. ( 4), the double Sumudu-Elzaki transform decomposition method, see Eq. ( 5), and double Sumudu-Aboodh transform, see Eq. ( 6).

Figure 2 Figure 3
Figure 2The comparison between the exact and numerical solutions for φ(χ, σ , t)

Figure 5
Figure 5The comparison between the exact and numerical solutions for ψ(χ, σ , t)

Figure 6 Figure 7
Figure 6The comparison between the exact and numerical solutions for φ(χ, σ , t)

Table 1
Comparison between the exact and approximation solutions for ψ(χ , σ , t)

Table 2
Comparison between the exact and approximation solutions for φ(χ , σ , t) Figure 1 The comparison between the exact and numerical solutions for ψ(χ, σ , t)Table 1 and Table 2 above show the comparison between exact and approximate solutions of Example 1.

Table 3 and
σ 2 e t , = χ 2σ 2 e t .Table4below shows the comparison between exact and approximate solutions of Example 2.

Table 3
Comparison between the exact and approximation solutions for ψ(χ , σ , t)

Table 4
Comparison between the exact and approximation solutions for φ(χ , σ , t)