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Exact Solution of Coupled Nonlinear PDEs Via Sumudu Decomposition Method

Sundas Rubab1, Jamshad Ahmad*1 and Muhammad Shakeel2 1

Department of Mathematics, Faculty of Sciences, University of Gujrat, Pakistan 2

Department of Mathematics, Mohi-ud-Din Islamic University, AJK, Pakistan

[email protected] (Jamshad Ahmad)

Abstract: In this paper, we apply the Sumudu Decomposition Method on system of coupled nonlinear partial differential equations to calculate the analytical solutions in closed form. The nonlinear term can easily be handled with the help of He’s polynomials. The proposed technique is tested on four problems. Calculated results show the potential of the technique. Keyword: Nonlinear PDEs, He’s polynomials, Sumudu transform, Adomian decomposition method

1. Introduction

Most of phenomena in nature are described by nonlinear differential equations. Different analytical methods have been applied to find a solution to them. For example, Adomian decomposition method has been applied for solving algebraic, differential, integro differential, differential-delay and partial differential equations. In the nonlinear case for ordinary differential equations and partial differential equations, the method has the advantage of dealing directly with the problem [1, 2]. These equations are solved without transforming them to more simple ones. The method avoids linearization, perturbation, discretization, or any unrealistic assumptions [3-5]. In the present paper, the intimate connection between the Sumudu transform theory and decomposition method arises in the solution of nonlinear partial

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Sumudu transform is defined over the set of the following functions: { ( ): 1, 2 0, ( )  / , (1) [0,)} j t t if Me t f t f A   j (1) by the following formula:

    0 2 1, ). ( , ) ( : ] ); ( [ ) (u S f t u f ut e dt u   G t (2)

In [6, 7], some fundamental properties of the Sumudu transform were established. In [8] this new transform was applied to the one-dimensional neutron transport equation. Further in [9] the Sumudu transform was extended to the distributions and some of their properties were also studied in [10]. Recently Ahmad et al. applied this transform to solve the fuzzy differential equations [11]. A very interesting fact about Sumudu transform is that the original function and its Sumudu transform have the same Taylor coefficients except a factor n i.e. !.

, ) ( 0

   n n nt a t f (3) and

   0 , ! ) ( n n nt a n u F (4)

Similarly, the Sumudu transform sends combinations,C(m,n), into permutations P(m,n), and hence it will be useful in the discrete systems. Further

. 1 )) ( ( )) ( ( , 1 )) ( ( )) ( ( u t S t H L t L t H S       (5)

Theorem: [12] let f(t) be in A, and let Gn(u)denote the Sumudu transform of the nth derivative fn(t) of f(t) then for n1

     1 0 . ) 0 ( ) ( ) ( n k k n k n n u f u u G u G (6)

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2. Analysis of the Method

We consider the general inhomogeneous nonlinear equation with initial conditions given below: ), , ( tx h NU RU LU   (7) where L is the highest order derivative which is assumed to be easily invertible, R is a linear differential operator of order less thanL,NU represents the nonlinear terms and h( tx, ) is the source term. First we explain the main idea of SDM, the method consists of applying Sumudu transform )]. , ( [ ] [ ] [ ] [LU S RU S NU S h x t S    (8) Using the differential property of Sumudu transform and initial conditions we get

)], , ( [ ] [ ] [ ) 0 , ( ... ) 0 , ( 1 ) 0 , ( 1 )] , ( [ 1 1 1 u S RU S NU S h x t x u x u u x u u t x u S u n n n n           (9) )] , ( [ ] [ ] [ ) 0 , ( ... ) 0 , ( ) 0 , ( )] , ( [u x t u x uu x u 1u 1 x u S RU u S NU u S h x t S      nn  nnn (10)

Assuming the solution as an infinite series

, ) , ( ) , ( 0 t x u p t x u i i i

   (11) and the nonlinear term can be decomposed as

, ) , ( 0

   i i H t x NU (12)

where H are He’s Polynomials ofi U , 0 U ,...1 U and it can be calculated by formula n

,... 2 , 1 , 0 , ] [ ! 1 0 0   

pu i N dp d i H p i i i i i i (13) Thus

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[ ] [ ( , )] [ ] [ ( , )]. ) 0 , ( ... ) 0 , ( ) 0 , ( ) , ( 0 2 1 1 0 t x h S u H S u t x RU S u RU S u x U u x U u x U t x U S n i i n n n n i i               

      (14) On comparing both sides and by using standard ADM

U0(x,t)

U(x,0) uU (x,0) ... u 1U 1(x,0) u S[h(x,t)] K(x,u),

S      nn  n  (15)

Then it follows that

]. [ )] , ( [ )] , ( [ ], [ )] , ( [ )] , ( [ 1 1 2 0 0 1 H S u t x RU S u t x U S H S u t x RU S u t x U S n n n n       (16)

In more general, we have

. 0 ], [ )] , ( [ )] , ( [U 1 x t u S RU x tu S H iS i n i n i (17)

On applying the inverse Sumudu transform

 

( , )

, 0, ) , ( ), , ( ) , ( 1 1 0        x t S u S RU x t u S H i U t x K t x U i n i n i (18)

where K( tx, )represents the term that is arising from source term and prescribed initial conditions. We now consider the inhomogeneous nonlinear partial differential equations:

)], , ( [ ] [ ] [ ] [LU S RU S NU S h x t S    (19) with the initial conditions

). ( ) 0 , ( ), ( ) 0 , (x f x u x g x ut  (20) Where 2 2 t L  

 is second-order differential operator, NU represents a general non-linear

differential operator where as h( tx, ) is source term. The methodology consists of applying Sumudu transform first on both sides,

)], , ( [ ] [ ] [ ) ( ) ( )] , ( [u x t f x ug x u2S RU u2S NU u2S h x t S      (21)

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[ ] [ ] [ ( , )]

. ) ( ) ( ) , (x t f x tg x S 1 u2S RU u2S NU u2S h x t u       (22) 3. Numerical Applications

Example3.1 Consider a nonlinear partial differential equation , 0 , 0 2 2    u u t utt x (23)

with initial conditions

. ) 0 , ( , 0 ) 0 , (x ut x ex u   (24) By taking Sumudu transform for (23) and (24), we obtain

], [ ) 0 , ( ) 0 , ( )] , ( [ 1 2 2 2 2 S u u u x u u x u t x u S u x t     (25) ], [ )] , ( [u x t ue u2S u2 u2 S x x    (26) applying the inverse Sumudu transform

[ ]

, ) , (x t te S 1 u2S u2 u2 ux  x  (27) which assumes a series solution of the function u( tx, )and is given by

   0 ). , ( ) , ( i i i t x u p t x u (28) Thus , ] ) ( ) ( [ ) , ( 0 0 2 1 0        

       i i i i x i i i u B u H S u S te t x u p (29) i

H And B are He’s polynomials that represent nonlinear terms. i

Thus by comparing the coefficients ofp , we get

x te t x u p0; 0( , ) , (30)  , 0 ] ) ( ) ( [ ) , ( ; 0 0 0 0 2 1 1 1        

     i i u B u H S u S t x u p (31)

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. 1 0 ] ) ( ) ( [ ) , ( ; 0 0 2 1 1 1        

       i u B u H S u S t x u p i i i i i i (32)

Therefore the exact solution when p1 is .

) ,

(x t tex

u  (33) Example 3.2 Consider the system of nonlinear coupled partial differential equation

. 5 ) , , ( , 5 ) , , ( , 1 ) , , (       y x t y x t y x t v u t y x w u w t y x v w v t y x u (34)

with initial conditions

. 2 ) 0 , , ( , 2 ) 0 , , ( , 2 ) 0 , , ( y x y x w y x y x v y x y x u        (35)

Applying the Sumudu transform we obtain

]. [ 5 ) 0 , , ( )] , , ( [ 1 ], [ 5 ) 0 , , ( )] , , ( [ 1 ], [ 1 ) 0 , , ( )] , , ( [ 1 y x y x y x v u S u y x w t y x w S u u w S u y x v t y x v S u w v S u y x u t y x u S u          (36) Then ]. [ 5 2 )] , , ( [ ], [ 5 2 )] , , ( [ ], [ 2 )] , , ( [ y x y x y x v u uS u y x t y x w S u w uS u y x t y x v S w v uS u y x t y x u S              (37)

By taking inverse Sumudu transform

[ ]

. 5 2 ) , , ( , ] [ 5 2 ) , , ( , ] [ 2 ) , , ( 1 1 1 y x y x y x v u uS S t y x t y x w u w uS S t y x t y x v w v uS S t y x t y x u                 (38)

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, 2 , 0 ] ) , ( [ ) , , ( ; , 0 ) , , ( ; , 2 ) , , ( ; , 2 ) , , ( ; 0 1 1 1 2 2 1 1 0 0              

     i w v H uS S t y x u p t y x u p t t y x u p y x t t y x u p i i i i  (39) , 2 , 0 ] ) , ( [ ) , , ( ; , 0 ) , , ( ; , 2 ) , , ( ; , 2 5 ) , , ( ; 0 1 1 1 2 2 1 1 0 0               

     i w u C uS S t y x v p t y x v p t t y x v p y x t t y x v p i i i i  (40) , 0 , 0 ] ) , ( [ ) , , ( ; , 0 ) , , ( ; , 2 ) , , ( ; , 2 5 ) , , ( ; 0 1 1 1 2 2 1 1 0 0               

     i v u B uS S t y x w p t y x w p t t y x w p y x t t y x w p i i i i  (41)

whereHi( wv, ), Ci(u,w) and Bi( vu, ) are Adomian polynomials representing the nonlinear

terms in above equations.

The solution of above system p1 is given by

. 3 2 ) , , ( , 3 2 ) , , ( , 3 2 ) , , ( t y x t y x w t y x t y x v t y x t y x u           (42)

Example 3.3 Consider the following homogeneous linear system of PDEs:

, 2 ) ( ) , ( ) , ( , 2 ) ( ) , ( ) , (         v u t x u t x v v u t x v t x u x t x t (43)

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. 1 ) 0 , ( , 1 ) 0 , (x ex v x ex u     (44) Taking the Sumudu transform

]. [ 2 ) 0 , ( )] , ( [ 1 ], [ 2 ) 0 , ( )] , ( [ 1 x x u v u S u x v t x v S u v u v S u x u t x u S u           (45) ]. [ 2 1 )] , ( [ ], [ 2 1 )] , ( [ x x x x u v u uS u e t x v S v u v uS u e t x u S              (46)

By taking inverse Sumudu transform

[ ]

. 2 1 ) , ( , ] [ 2 1 ) , ( 1 1 x x x x u v u uS S t e t x v v u v uS S t e t x u                (47)

     0 0 ). , ( ) , ( ), , ( ) , ( i i xi i x xi i x x t pu x t v x t p v x t u (48)

Using the decomposition seriesu( tx, ),v( tx, )and u ,x v for the linear terms, we obtain x

. ] [ 2 1 ) , ( , ] [ 2 1 ) , ( 0 0 0 1 0 0 0 0 1 0                       

                  i i i ix i i i i i x i i i i i i i i i ix i i x i i i v p u p u p uS S t e t x v p v p u p v p uS S t e t x u p (49)

Thus recursive relation is

 , ! 2 ) , ( ; , 2 ) , ( ; , 2 1 ) , ( ; 2 2 2 1 1 0 0 x x x e t t x u p t te t x u p t e t x u p       (50)  , ! 2 ) , ( ; , 2 ) , ( ; , 2 1 ) , ( ; 2 2 2 1 1 0 0 x x x e t t x v p t te t x v p t e t x v p         (51)

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...). ! 3 ! 2 1 ( 1 ) , ( ...), ! 3 ! 2 1 ( 1 ) , ( 3 2 3 2              t t t e t x v t t t e t x u x x (52)

Thus the solutions

. 1 ) , ( , 1 ) , ( t x t x e t x v e t x u        (53)

Example 3.4 Consider the system of nonlinear partial differential equations

, 1 , 1       v uv v u vu u x t x t (54) with initial conditions

x

e x

u( ,0) ,v(x,0)ex. (55)

By taking Sumudu transform on the Eq. (54)

( , )

( ,0) 1

, 1 , 1 ) 0 , ( ) , ( 1 v uv S u x u u x v S u u vu S u x u u x u S u x x         (56)

Using initial conditions:

( , )

[ ] [ ], ], [ ] [ ) , ( v uS uv uS u e u x v S u uS vu uS u e u x u S x x x x          (57)

By taking inverse Sumudu transform

[ ]

, ) , ( , ] [ ) , ( 1 1 v uv uS S t e t x v u vu uS S t e t x u x x x x            (58) Then we can write u( tx, )and v( tx, ) as an infinite series:

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, ) , ( , ) , ( 0 0 1 0 0 0 1 0                              

               i i i i x i i i i i i i x i i i v B uS S t e t x v p u H uS S t e t x u p (59)

That represent the nonlinear terms vu and x uv respectively. x

By comparing the coefficients ofp, we get

, ; , ; 0 0 0 0 t e v p t e u p x x      (60)

, ! 2 ! 2 ; , ! 2 ! 2 ; 2 2 0 0 1 1 1 2 2 0 0 1 1 1 x x x x e t te t t v B uS S v p e t te t t u H uS S u p                     (61)

..., ! 2 ! 2 ; ..., ! 2 ! 2 ; 2 2 2 2 1 2 2 2 2 2 2 1 2 2 x x e t t v B uS S v p e t t u H uS S u p               (62) , Thus . ... ! 3 ! 2 1 ) , ( , ... ! 3 ! 2 1 ) , ( 3 2 3 2                      t t t e t x v t t t e t x u x x (63)

Then the solution for the above system is as follows:

t x e t x u( , )  , v(x,t)etx. (64)

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4. Conclusion

The Sumudu Decomposition Method has been applied successfully to linear and nonlinear systems of partial differential equations. Four examples have been presented. The obtained results show that the proposed method is very useful and reliable for nonlinear partial differential equation and systems. Therefore, this method can be applied to many complicated nonlinear problems arising in mathematical physics and engineering.

References

[1] G. Adomian, Solving Frontier Problems of Physics: The Decomposition Method, Kluwer Academic Publishers, Boston, MA, 1994.

[2] Adomian G, A review of the decomposition method in applied mathematics, J. Math. Anal. Appl. 135, 1988, 501–544.

[3] M. Dehghan and M. Tatari, Solution of a semilinear parabolic equation with an unknown control function using the decomposition procedure of Adomian, Num. Meth. Par. Diff. Eq., 23 (2007), 499-510.

[4] J. Ahmad et al, Analytical Exact Solution of Advection Problems via Coupling of Sumudu Decomposition Method and Taylor’s Series, International Journal of Hybrid Information Technology, Vol.8, No.4 (2015), pp.117-124.

[5] J. Ahmad, S. Rubab, M. Naeem and L.A. Tahir, Applications of Sunmudu decomposition method to Goursat problems, Journal of Science and Arts, 4(29), 287-298 (2014).

[6] M. A. Asiru, Sumudu transform and the solution of integral equations of convolution type, International Journal of Mathematical Education in Science and Technology, vol. 32, no. 6, 906–910, 2001.

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[7] M. A. Asiru, Further properties of the Sumudu transform and its applications, International Journal of Mathematical Education in Science and Technology, vol. 33, no. 3, 441–449, 2002.

[8] A. Kadem and A. Kılıc¸man, Note on transport equation and fractional Sumudu transform, Computers & Mathematics with Applications, vol. 62, no. 8, 2995–3003, 2011.

[9] H. Eltayeb, A. Kılıc¸man, and B. Fisher, A new integral transform and associated Integral Transforms and Special Functions, vol. 21, no. 5, 367–379, 2010.

[10] A. Kılıc¸man and H. Eltayeb, On the applications of Laplace and Sumudu Journal of the Franklin Institute, vol. 347, no. 5, pp. 848–862, 2010.

[11] M.Z. Ahmad and N.A. Abdul Rahman, Explicit solution of fuzzy differential equations by mean of fuzzy Sumudu transform. Int. J. Appl. Phys. Math. 2015, 5, 86– 93.

[12] A. Kılıc¸man, H. Eltayeb, and K. A. M. Atan, A note on the comparison between Laplace Sumudu transforms, Bulletin of the Iranian Mathematical Society, vol. 37, no. 1, 131–141, 2011.

References

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