亚洲免费av电影一区二区三区,日韩爱爱视频,51精品视频一区二区三区,91视频爱爱,日韩欧美在线播放视频,中文字幕少妇AV,亚洲电影中文字幕,久久久久亚洲av成人网址,久久综合视频网站,国产在线不卡免费播放

        ?

        New Jacobi Elliptic Function Solutions for the Generalized Nizhnik-Novikov-Veselov Equation?

        2012-12-27 07:05:30HONGBAOJIAN

        HONG BAO-JIAN

        (Department of Basic Courses,Nanjing Institute of Technology,Nanjing,211167)

        New Jacobi Elliptic Function Solutions for the Generalized Nizhnik-Novikov-Veselov Equation?

        HONG BAO-JIAN

        (Department of Basic Courses,Nanjing Institute of Technology,Nanjing,211167)

        In this paper,a new generalized Jacobi elliptic function expansion method based upon four new Jacobi elliptic functions is described and abundant solutions of new Jacobi elliptic functions for the generalized Nizhnik-Novikov-Veselov equations are obtained.It is shown that the new method is much more powerful in finding new exact solutions to various kinds of nonlinear evolution equations in mathematical physics.

        generalized Jacobi elliptic function expansion method,Jacobi elliptic function solution,exact solution,generalized Nizhnik-Novikov-Veselov equation

        1 Introduction

        In recent years,due to the wide applications of soliton theory in natural science,searching for exact soliton solutions of nonlinear evolution equations plays an important and signi ficant role in the study on the dynamics of those phenomena(see[1]).Particularly,various powerful methods have been presented,such as inverse scattering transformation,Cole-Hopf transformation,Hirota bilinear method,homogeneous balance method,Backlund transformation,Darboux transformation,projective Riccati equations method and so on.In this paper,we discuss a generalized Nizhnik-Novikov-Veselov(GNNV)equation by our generalized Jacobi elliptic function expansion method(see[2])proposed recently.As a result,more new exact solutions are obtained.The character feature of our method is that,without much extra e ff ort,we can get series of exact solutions by using a uniform way.Another advantage of our method is that it also applies to general higher-dimensional nonlinear partial differential equations.

        We consider the following GNNV equations(see[3–6]):

        where a,b,c and d are arbitrary constants.For

        the GNNV equations(1.1)are degenerated to the usual two-dimensional NNV equations (see[7–8]),which is an isotropic Lax extension of the classical(1+1)-dimensional shallow water-wave KdV model.When

        we get the asymmetric NNV equation,which may be considered as a model for an incompressible fl uid.Some types of exact solutions of the GNNV equations have been studied in recent years(see[9–13]).

        2 Summary of the New Generalized Jacobi Elliptic Functions Expansion Method

        Given a partial differential equation with three variables x,y and t

        we seek the following formal solutions of the given system by a new intermediate transformation:

        where A0,Ai,Bi,Ci,Di(i=1,2,···,n)are constants to be determined later,ξ=ξ(x,y,t) is an arbitrary function with the variables x,y and t,the parameter n can be determined by balancing the highest order derivative terms with the nonlinear terms in(2.1),and E(ξ), F(ξ),G(ξ),H(ξ)are the arbitrary arrays of the four functions

        respectively.The selection obeys the principle which makes the calculation more simple. We ansatz

        where p,q,r,l are arbitrary constants which ensure denominator unequal to zero,so do the following situations.The four functions e,f,g,h satisfy the following restricted relations:

        Substituting(2.4)along with(2.5a)–(2.5d)into(2.1),respectively,yields four families of polynomial equations for E(ξ),F(ξ),G(ξ),H(ξ).

        Setting the coefficients of Fi(ξ)Ej1(ξ)j2G(ξ)j3H(ξ)j4(i=0,1,2,···;j1,j2,j3,j4=0,1; j1j2j3j4=0)to be zero yields a set of over-determined differential equations in A0,Ai,Bi, Ci,Di(i=1,2,···,n)and ξ(x,y,t).Solving the over-determined differential equations by Mathematica and Wu elimination,we obtain many exact solutions of(2.1)accroding to (2.2)and(2.3).

        Obviously,if we choose the special values of p,q,r,l,m in(2.3),then we can get the results in[13–16],which has been discussed in[2].

        3 Exact Solutions to the Generalized Nizhnik-Novikov-Veselov Equation

        To seek the traveling wave solutions of(1.1),we make the gauge transformation

        where k,τ,ω are constants to be determined later,and ξ0is an arbitrary constant.

        Substituting(3.1)into(1.1)yields the ordinary differential equations(ODEs)of u(ξ), v(ξ),w(ξ)and integrating these ODEs makes the equations(1.1)to become

        where C1and C2are integral constants.By balancing the highest-order of the linear term u′′and the nonlinear term u2in(3.2a),we obtain n=2.Thus we assume that(3.2a)has the following solutions:

        satisfy(2.4)and(2.5a)–(2.5d).Substituting(2.4)and(2.5a)–(2.5d)along with(3.3)into (3.2a),respectively,and setting the coefficients of Fi(ξ)Ej1(ξ)j2G(ξ)j3H(ξ)j4(i=0,1,2,···; j1,j2,j3,j4=0,1;j1j2j3j4=0)to be zero yield an ODEs with respect to the unknowns ci(i=0,···,4),dj(j=1,···,10),ω,k,τ,p,q,r,l.After solving the ODEs by Mathematica and Wu elimination,we determine the following solutions:

        Family 1: For p=0,we have

        Case 1.

        where k,τ,ξ0,c0,C1are arbitrary constants.ci(i=1,···,4)and dj(j=1,···,10)not mentioned here are zero,so do the following situations.

        Therefore,from(2.3),(3.1),(3.3)and Case 1,we obtain the following solutions to the GNNV equations(1.1):

        With the same process we derive the other three families of new exact solutions of(1.1), where

        Remark 3.1Solutions u1,u6,u7,u8degenerate to solitary solutions when the modulus m → 1,and solutions u1,u3,u5,u7,u8degenerate to triangular function solutions when the modulus m→0.Here u6is just the solutions u1,u2,u3in[1].The other seven types of explicit solutions to(1.1)we obtained are not shown in the previous literature to our knowledge.

        4 Conclusion

        In this paper,we propose an approach for finding the new exact solutions for the nonlinear evolution equations by constructing the four new types of Jacobi elliptic functions(2.3). By using this method and computerized symbolic computation,we have found abundant new exact solutions of(1.1).More importantly,our method is much simple and powerful for finding new solutions to various kinds of nonlinear evolution equations.We believe that this method should play an important role in finding the exact solutions in mathematical physics.

        [1]Ablowitz M J,Clarkson P A.Solitons,Nonlinear Evolution Equations and Inverse Scattering. New York:Cambridge Univ.Press,1991.

        [2]Hong B J.New Jacobi elliptic functions solutions for the variable-coefficient mKdV equation.Appl.Math.Comput.,2009,215:2908–2913.

        [3]Zhang J L,Ren D F,Wang M L,Wang Y M,Fang Z D.The periodic wave solutions for the generalized Nizhnik-Novikov-Veselov equation.Chinese Phys.,2003,12:825–830.

        [4]Peng Y Z.A class of doubly periodic wave solutions for the generalized Nizhnik-Novikov-Veselov equation.Phys.Lett.A,2005,337:55–60.

        [5]Borhanifar A,Kabir M M,Maryam L V.New periodic and soliton wave solutions for the generalized Zakharov system and(2+1)-dimensional Nizhnik-Novikov-Veselov system.Chaos Solitons Fractals,2009,42:1646–1654.

        [6]Zhang Y Y,Zhang Y,Zhang H Q.New complexiton solutions of(2+1)-dimensional Nizhnik-Novikov-Veselov equations.Comm.Theoret.Phys.,2006,46:407–414.

        [7]Nizhnik L P.Integration of multidimensional nonlinear equations by the method of the inverse problem.Soviet Phys.Dokl.,1980,25:706–708.

        [8]Novikov S P,Vesslov A P.Two-dimensional Schrdinger operator:inverse scattering and evolutional equations.Phys.D.,1986,18:267–273.

        [9]Boiti M,Leon J P,Manna M,Pempinelli F.On the spectral transform of a Korteweg-de Vries equation in two spatial dimensions.Inverse Problems,1986,2:271–279.

        [10]Radha R,Lakshmanan M.Singularity structure analysis and bilinear form of a(2+1)-dimensional nonlinear NLS equation.Inverse Problems,1994,35:4746–4756.

        [11]Yu G F,Tam H W.A vector asymmetrical NNV equation:soliton solutions,bilinear Backlund transformation and Lax pair.J.Math.Anal.Appl.,2008,344:593–600.

        [12]Wazwaz A M.New solitary wave and periodic wave solutions to the(2+1)-dimensional Nizhnik-Novikov-Veselov system.Appl.Math.Comput.,2007,187:1584–1591.

        [13]Deng C F.New abundant exact solutions for the(2+1)-dimensional generalized Nizhnik-Novikov-Veselov system.Comm.Nonlinear Sci.Numer.Simul.,2010,15:3349–3357.

        [14]Chen H T,Yin H C.A note on the elliptic equation method.Comm.Nonlinear Sci.Numer. Simul.,2008,13:547–553.

        [15]Wang Q,Chen Y,Zhang H Q.An extended Jacobi elliptic function rational expansion method and its application to(2+1)-dimensional dispersive long wave equation.Phys.Lett.A,2005, 340:411–426.

        [16]Lu D C,Hong B J.New exact solutions for the(2+1)-dimensional generalized Broer-Kaup System.Appl.Math.Comput.,2008,199:572–580.

        Communicated by Yin Jing-xue

        35J20,35Q25

        A

        1674-5647(2012)01-0043-08

        date:Sept.14,2009.

        The Scienti fi c Research Foundation(QKJA2010011)of Nanjing Institute of Technology.

        亚洲av无码专区在线播放| 中文字幕一区二区网址| 日本免费一区二区三区在线播放| 无码熟妇人妻av影音先锋| 亚洲欧美日韩在线一区| 久久精品国产72国产精福利| 亚洲av一二三四五区在线| 精品久久久久久无码专区| 黑人玩弄人妻中文在线| 96精品免费视频大全| 中文字幕人妻互换激情| 丁香婷婷激情综合俺也去| 日韩欧美在线综合网| 特级毛片全部免费播放a一级| 中文字幕av素人专区| 国产亚洲精品久久久闺蜜| 日本55丰满熟妇厨房伦| 青青草一级视频在线观看| 少妇免费av一区二区三区久久 | 国产一区二区三区中出| 欧美人与善在线com| 国产欧美亚洲精品a| 亚洲国产AⅤ精品一区二区不卡| 日韩在线不卡一区三区av| 国产午夜精品av一区二区麻豆| 亚洲男人天堂| 久久精品有码中文字幕1| 日本免费一区二区三区影院 | 97久久精品人人做人人爽| 永久免费毛片在线播放| 日本少妇一区二区三区四区| 色爱无码av综合区| 亚洲熟妇一区无码| 国产超碰在线91观看| 国产精品爽爽ⅴa在线观看| 学生妹亚洲一区二区| 国产偷闻隔壁人妻内裤av| 亚洲乱码av中文一区二区| 先锋影音av最新资源| 亚洲中文欧美日韩在线| 亚洲乱妇熟女爽到高潮视频高清|