LIU Shao-qing,GAO Guo-cheng
(Department of Basic Courses,Shandong University of Science and Technology,Jinan 250031,China)
Exact Solutions of the Wick-type KdV-Burgers Equation
LIU Shao-qing,GAO Guo-cheng
(Department of Basic Courses,Shandong University of Science and Technology,Jinan 250031,China)
In this paper,we consider the wick-type KdV-Burgers equation with variable coefficients.By using Tanh method with the aid of Hermite transformation,we deduce the exact solutions which include hyperbolic-exponential,trigonometric-exponential and exponential function solutions for the considered equation.
stochastic partial differential equation;Tanh method;exact solutions
2000 MR Subject Classification:35Q20
Article ID:1002—0462(2016)02—0139—08
Chin.Quart.J.of Math.
2016,31(2):139—146
In the 1980s,Wadati[13]first introduced and studied stochastic KdV equations.From then on,more and more scholars begin to pay close attention to this kind of equation and get a lot of valuable research results[49].Compared with other partial differential equation,the solutions of the stochastic partial differential equations(SPDEs)are more difficult to find.Since 1996,Holden et al[10]has studied Wick stochastic partial differential equation using white noise analysis.Then more and more researches about the exact solution of the SPDEs appear.In 2003,Xie[11]studied stochastic KdV equation with the homogeneous balance method to obtain a lot of random solitary wave solution and then used the same method to study stochastic mKdV equations,stochastic Kadomtsev-Petviashvili equation and 2-dimension stochastic KdV equations[1214].Subsequently,Chen et al[1516]studied the generalized stochastic Hirota-Satsuma and stochastic nonlinear Schr¨odinger equation with F-expansion method.Liu and others[1719]studied stochastic mKdV equations and stochastic KdV equation by mapping method.In 2007,Liu[20]studied the stochastic KdV equations using Jacobi ellipticfunction method,then studied the generalized stochastic KdV equations using Tanh function method[21].Kim and others[22]studied generalized stochastic Boussinesq equations and stochastic Kadomtsev-Petviashvili equation with-expansion method.
In this paper,we will deduce three types of the exact solutions to the generalized stochastic KdV-Burgers equation
Ut+H1(t)ƒ(Uxxx+6U ƒ Ux)+4H2(t)ƒ Ux-H3(t)ƒ(2U+xUx)+H4(t)ƒ Uxx=0,(1.1)where ƒ stands for the Wick product on the Hida distribution space(S(R))∗and Hi(t)(i= 1,2,3)are the white noise.
Let(S(Rd))and(S(Rd))∗be the Hida test function space and the Hida distribution space on Rd.We first introduce some concepts about the Wick type.The Wick product X ƒ Y of two elementsis defined by X ƒ Y=
Suppose that modeling considerations lead us to consider an SPDE expressed formally as
where A is some given function,U=U(t,x,ω)is the unknown(generalized)stochastic process, and where the operatorswhen x=(x1,x2,···,xd)∈Rd.
First we interpret all products as Wick products and all functions as their Wick versions,We indicate this as
Secondly,we take the Hermite transform of(2.2).This turns Wick products into ordinary products and the equation takes the form
foreachz=(z1,z2,···)∈forsomeq,r,where<r2.
Then,under certain conditions,we can take the inverse Hermite transform U=H-1(u)∈(S)-1and thereby obtain a solution U of the original(Wick)equation(2.2).We have the following theorem,which was proved by Holden et al[10].
Theorem 2.1Suppose u(t,x,z)is a solution(in the usual strong,pointwise sense)of the equation(2.4)for(t,x)in some bounded open set G⊂R×Rdand for all z∈KRq,for some q,R.Moreover,suppose that u(t,x,z)and all its partial derivatives,which are involved in(2.4)are(uniformly)bounded for(t,x,z)∈G×KRq,continuous with respect to(t,x)∈G for each z∈KRqand analytic with respect to z∈KRq,for all(t,x)∈G.
Then there exists U(t,x)∈(S)-1such that u(t,x,z)=(HU(t,x))(z)=(eU(t,x))(z)for all(t,x,z)∈G×KRqand U(t,x)solves(in the strong sense in(S)-1)the equation(2.1)in(S)-1.
Consider the wick-type SPDE(2.2)
Step 1By the Hermite transform,we transform(2.2)into an ordinary equation(2.3). Considering the transformation˜U(t,x,z)=u(t,x,z)=u(ξ),we reduce the equation(2.3)into
Step 2We suppose that equation(3.1)has the following forms of solution
where ai=ai(x2,x3,···,xd,z,t),i=0,1,···,M,ξ=ξ(x1,x2,···,xd,z,t)are functions to be determined and ψ(ξ)satisfies
so we can easily know that(3.3)has the following solutions
Step 3Substituting(3.2)and(3.3)into(3.1)and then setting the coefficients of xkψi(ξ)of the resulting equation to zero,we can obtain an over-determined system of algebraic equations with respect to a1,···,aM,ξ.Then we solve the above system and get the specific forms of these unknown parameters.
Step 4Substituting the result of Step 3 into(3.2)along with(3.4)~(3.6),we can get the exact solutions u(t,x,z)of(3.1).
Step 5Taking the inverse Hermite transformation of u(t,x,z)obtained in Step 4,i.e.,U(t,x)=H-1(u(t,x,z)),we get the solutions of the wick-type stochastic equation(2.2).
In this section,we will give exact solutions of(1.1).Taking the Hermite transform of(1.1),we can get the equation
where U depend on t,x and z,eHi,i=1,2,3,4 depend on t and z,z=(z1,z2,···)∈(CN)is a vector parameter.
For the sake of simplicity,we denote u(t,x,z)=eU(t,x,z),Hi(t,z)=eHi(t,z),i=1,2,3,4,so(4.1)becomes
Now let us use the Tanh function method and look for solutions as
where f(t,z),g(t,z)are functions to be determined later.
We consider that the solutions of the equation(4.2)can be expressed in the form
where ai(t,z)are functions to be determined later.M is a positive integer that can be determined by balancing the differential term of highest order with the nonlinear term in(4.2).ψ(ξ)satisfies the equation(3.3).Then,balancing the linear term of highest order with the nonlinear term in the equation(4.2)leads to set
substituting(3.3)and(4.5)into(4.2)and setting the coefficients of xkψi(ξ)to zero,the following system of equations arises
From(4.6)~(4.10),we can obtain
substituting(4.16)and(4.17)into(4.11),we have
According(4.13)and(4.15),we get
When H24(t,z)=100bH21exp(2RtH3(s,z)ds),(4.16)~(4.20)naturally satisfy(4.12)and(4.14). Therefore we get the solution of equation(4.2)as follows
where
Suppose that h(t)is an integrable function on R+and
we have
where bi,i=1,2,3 are arbitrary constant,W(t)is Gauss white noise and B(t)is Brownian motion.We know W(t)=˙B(t).
Considering the Hermite transformation of(4.23)and(4.24),we have
where
According to Theorem 1 and expƒ,we obtain the generalized stochastic solution
where
andR(·)δB(t)is the Skorohod integral.
Substituting(3.4)~(3.6)into(4.29)and(4.30),we can get three types of the exact solutions.
(1)The functional solutions of hyperbolic-exponential type(b>0)
where
(2)The functional solutions of trigonometric-exponential type(b<0)
where
(3)The functional solution of exponential type(b=0)
where
We successfully discussed the solutions of the nonlinear stochastic equation with Gaussian white noise.Three types of the exact solutions are obtained which include hyperbolicexponential,trigonometric-exponential exponential function solutions.
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O175.2Document code:A
date:2014-04-03
Supported by the National Natural Science Foundation of China(11271008,61072147)
Biographies:LIU Shao-qing(1977-),female,native of Qingdao,Shandong,a lecturer of Shandong University of Science and Technology,Ph.D.,engages in soliton and integrable system;GAO Guo-cheng(1963-),male,native of Xinyang,Henan,a professor of Shandong University of Science and Technology,M.S.D.,engages in control theory and optimization.
Chinese Quarterly Journal of Mathematics2016年2期