<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2014.23005</article-id><article-id pub-id-type="publisher-id">JAMP-43178</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Application of Trial Equation Method for Solving the Benjamin Ono Equation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ang</surname><given-names>Li</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Northeast Petroleum University, Daqing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>liyang120918@163.com</email></corresp></author-notes><pub-date pub-type="epub"><day>10</day><month>02</month><year>2014</year></pub-date><volume>02</volume><issue>03</issue><fpage>45</fpage><lpage>49</lpage><history><date date-type="received"><day>January</day>	<month>7,</month>	<year>2014</year></date><date date-type="rev-recd"><day>February</day>	<month>7,</month>	<year>2014</year>	</date><date date-type="accepted"><day>February</day>	<month>15,</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
   In the article, the nonlinear equation is reduced to an ordinary differential equation under the travelling wave transformation. Using trial equation method, the ODE is reduced to the elementary integral form. In the end, complete discrimination system for polynomial is used to solve the corresponding integrals and obtain the classification of all single travelling wave solutions to the equation. 
 
</p></abstract><kwd-group><kwd>The Nonlinear Partial Differential Equation; Complete Discrimination System for Polynomial; Trial Equation Method; Traveling Wave Transform; The Benjamin Ono Equation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Nonlinear phenomena are general problems in every field of engineering technology, science research, natural world and human society activities. So the investigation of exact solutions of nonlinear equations plays a important role not only in theoretic research but in application. To obtain the travelling wave solutions, many methods were attempted, such as the inverse scattering method [<xref ref-type="bibr" rid="scirp.43178-ref1">1</xref>], Hirotas bilinear transformation [2,3], the tanh method [<xref ref-type="bibr" rid="scirp.43178-ref4">4</xref>], sine-cosine method [<xref ref-type="bibr" rid="scirp.43178-ref5">5</xref>], homogeneous balance method [6,7], exp-function method [<xref ref-type="bibr" rid="scirp.43178-ref8">8</xref>], and so on. These methods derived many solutions to most nonlinear evolution equations. Recently, Professor Liu proposed a powerful method named trial equation method for finding exact solutions to nonlinear differential equations [9-11]. By using his method, the nonlinear differential equation is reduced to an ordinary differential equation under the travelling wave transformation. Using the trial equation method, the ODE is reduced to the elementary integral form. In the end, the complete discrimination system for polynomial is used to solve the corresponding integrals. We can obtain the classification of all single travelling wave solutions [12-16] to the equation. This idea is so good that many types of nonlinear differential equations can be solved by it. Using the trial equation method and complete discrimination system for polynomial, we have obtained a lot of new solutions to many nonlinear differential equations. As an application, some new solutions to the Benjamin Ono equation are given.</p></sec><sec id="s2"><title>2. Application of the Trial Equation Method</title><p>The Benjamin Ono equation reads as</p><disp-formula id="scirp.43178-formula106906"><label>(1)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\e307a66b-40f9-4ccc-a872-ca3570b7286f.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\eeac1e65-456b-4b01-b4a9-ff450a59c6c8.png" xlink:type="simple"/></inline-formula> are parameters.Taking the traveling wave transformation <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\05dd622d-679b-44e4-a6bf-7a22b9ddfffe.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\57a7d56e-0d59-49ab-a57b-47257be24f6d.png" xlink:type="simple"/></inline-formula>, we can obtain the corresponding reduced ODE.</p><disp-formula id="scirp.43178-formula106907"><label>(2)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\f1b10af9-5418-478d-aeb3-e5cf6bdb70f0.png"  xlink:type="simple"/></disp-formula><p>we take the trial equation as follows:<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\42521615-428a-470f-a26c-05374976a599.png" xlink:type="simple"/></inline-formula>.</p><p>According to the trial equation method of rank homogeneous equation, balancing <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\4f1550b5-4391-4fe0-82ca-d5d1429c5120.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\d5fc5aa0-4d1c-4c93-97f3-c2b9651471f6.png" xlink:type="simple"/></inline-formula> (or<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\d5d53304-3428-4e31-b175-24caff706cf1.png" xlink:type="simple"/></inline-formula>) gets<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\5f46f19a-55d2-4254-af89-99bf4212556e.png" xlink:type="simple"/></inline-formula>. Equation (4) has the following specific form</p><disp-formula id="scirp.43178-formula106908"><label>(3)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\7c195ad3-deb4-4f43-aaf2-016f7ef1312d.png"  xlink:type="simple"/></disp-formula><p>Integrating the Equation (3)once with respect to<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\30a85843-1679-4511-a48f-a92359c3b9ac.png" xlink:type="simple"/></inline-formula>, we get</p><disp-formula id="scirp.43178-formula106909"><label>(4)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\3fb71ab0-d240-46fd-a8e2-3101e5225a3c.png"  xlink:type="simple"/></disp-formula><p>By Equation (3) and Equation(4), we derive the following equation</p><disp-formula id="scirp.43178-formula106910"><label>(5)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\13be988b-097c-44af-840f-5f7dbc0ad386.png"  xlink:type="simple"/></disp-formula><p>Substituting Equations (3)-(5) into Equation (2), we have</p><disp-formula id="scirp.43178-formula106911"><label>(6)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\77b2a0bf-d6b2-4ba9-99af-e73f62c0ba0c.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.43178-formula106912"><label>(7)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\15b811b4-ecd5-4041-b70e-ef6065982c15.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.43178-formula106913"><label>(8)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\256465d5-b621-475f-a2a8-b55c87667896.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.43178-formula106914"><label>(9)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\cf3576cd-4e65-4171-b0c2-e1bb4a950e0a.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.43178-formula106915"><label>(10)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\3e77ebeb-57d9-419a-8c45-c0170c4219b7.png"  xlink:type="simple"/></disp-formula><p>Let the coefficient <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\3cbb116a-0182-4a5c-8ead-e94edb1a01b1.png" xlink:type="simple"/></inline-formula> be zero,we will yield nonlinear algebraic equations.Solving the equations, we will determine the values of<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\4b350c2d-c025-4838-9eca-82b2207103ce.png" xlink:type="simple"/></inline-formula>.</p><p>We get <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\fece9e19-4469-4f75-8da1-1e5df207824d.png" xlink:type="simple"/></inline-formula> and d are two arbitrary constants. When the above conditions are satisfied, we use the complete discrimination system for the third order polynomial and have the following solving process.</p><p>Let</p><disp-formula id="scirp.43178-formula106916"><label>(11)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\802acea6-2294-4e36-8242-883639ffe359.png"  xlink:type="simple"/></disp-formula><p>Then Equation(4) becomes</p><disp-formula id="scirp.43178-formula106917"><label>(12)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\c1a28a2c-4c69-458c-b55b-cd4114e2f06d.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\8de1e214-c762-40ed-a9a9-d71d41f32c2d.png" xlink:type="simple"/></inline-formula> is a function of<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\6c1d4bbf-c32c-41f5-b41a-c91411d8d1e5.png" xlink:type="simple"/></inline-formula>.The integral form of Equation(12) is</p><disp-formula id="scirp.43178-formula106918"><label>(13)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\da6d90e2-3911-40d0-8171-13ddf885273b.png"  xlink:type="simple"/></disp-formula><p>Denote</p><disp-formula id="scirp.43178-formula106919"><label>(14)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\25cf3c4e-2c2d-4bd6-b265-76aa347a54f2.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.43178-formula106920"><label>(15)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\ea31b5ad-ed73-44b2-ab9c-82d6927aa2ae.png"  xlink:type="simple"/></disp-formula><p>According to the complete discrimination system, we give the corresponding single traveling wave solutions to Equation(1).</p><p>Case 1. <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\5764f43e-4acb-4838-822d-259b55ff6fd1.png" xlink:type="simple"/></inline-formula>has a double real root and a simple real root. Then we have</p><disp-formula id="scirp.43178-formula106921"><label>(16)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\0b9c0d9d-ea0a-4613-bdb0-6edccc0192bc.png"  xlink:type="simple"/></disp-formula><p>when<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\43150556-2fb0-42be-be98-342e83dad102.png" xlink:type="simple"/></inline-formula>, the corresponding solutions are</p><disp-formula id="scirp.43178-formula106922"><label>(17)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\16162c6a-64cc-48cb-8af7-4b47f745f7ab.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.43178-formula106923"><label>(18)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\a2ef0b2b-f391-47f2-8a3e-eecb6dc3a712.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.43178-formula106924"><label>(19)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\e985f0ae-b0a4-4ed5-b895-fb58f70f738a.png"  xlink:type="simple"/></disp-formula><p>Case 2. <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\b64bff75-ad5e-411c-aff0-8e0a159dca8c.png" xlink:type="simple"/></inline-formula>has a triple root. Then we have</p><disp-formula id="scirp.43178-formula106925"><label>(20)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\8c8f29f8-5c7c-4670-b05a-cf6a6f6b8c16.png"  xlink:type="simple"/></disp-formula><p>The corresponding solution is</p><disp-formula id="scirp.43178-formula106926"><label>(21)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\a15ac3bb-882a-4686-a5f2-dd198252e19f.png"  xlink:type="simple"/></disp-formula><p>Case 3. <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\7306806d-242b-4242-a4b1-960291812212.png" xlink:type="simple"/></inline-formula>has three different real roots. Then we have</p><disp-formula id="scirp.43178-formula106927"><label>(22)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\5a895f2c-6407-4cd3-b3c1-2d76ad95c2da.png"  xlink:type="simple"/></disp-formula><p>when<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\c27a6c62-8509-4503-8423-3dcabdf3fa34.png" xlink:type="simple"/></inline-formula>, we take the transformation as follows</p><disp-formula id="scirp.43178-formula106928"><label>(23)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\730a979e-5bfd-46d5-93e2-1ebb9935f4f5.png"  xlink:type="simple"/></disp-formula><p>According to the Equation(12), we have</p><disp-formula id="scirp.43178-formula106929"><label>(24)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\465d5bb5-7cda-4251-a046-23cf70e89c7f.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\7426e066-7e03-4234-9118-bc6ff2983150.png" xlink:type="simple"/></inline-formula>.On the basis of the Equation(24) and the definition of the Jacobi elliptic sine function, we have</p><disp-formula id="scirp.43178-formula106930"><label>(25)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\1db47502-e362-4dac-b52c-cd99d739a22d.png"  xlink:type="simple"/></disp-formula><p>The corresponding solutions is</p><disp-formula id="scirp.43178-formula106931"><label>(26)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\a6fa1a0a-9455-4eda-9d70-666a0c7747a3.png"  xlink:type="simple"/></disp-formula><p>when<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\d9673c66-8eef-4a14-a4db-b511303f968c.png" xlink:type="simple"/></inline-formula>, we take the transformation as follows</p><disp-formula id="scirp.43178-formula106932"><label>(27)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\53c5ee61-282f-40c5-b8cb-674b1ecfc675.png"  xlink:type="simple"/></disp-formula><p>The corresponding solutions is</p><disp-formula id="scirp.43178-formula106933"><label>(28)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\9d6f259a-fb70-4c16-bceb-14649d16dad2.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\2266c80b-bfef-4a91-943e-09bc91202828.png" xlink:type="simple"/></inline-formula>.</p><p>Case 4. <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\9bd26edf-67b2-46db-934d-2e81750b91a9.png" xlink:type="simple"/></inline-formula>has only a real root. Then we have</p><disp-formula id="scirp.43178-formula106934"><label>(29)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\3f4ad767-76b0-40f8-88aa-6d75f69c268b.png"  xlink:type="simple"/></disp-formula><p>when<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\fbc588ac-f7fa-41a4-83e3-5fcfd405cacb.png" xlink:type="simple"/></inline-formula>, we take the transformation as follows</p><disp-formula id="scirp.43178-formula106935"><label>(30)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\d6b04496-7ac5-4dd6-9f11-1b402ffcb85b.png"  xlink:type="simple"/></disp-formula><p>According to the Equation(13), we have</p><disp-formula id="scirp.43178-formula106936"><label>(31)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\f83cffba-294c-405c-b841-426a4646177d.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\2ac33cde-cb7e-4ba3-a040-d31d01f87a17.png" xlink:type="simple"/></inline-formula>. On the basis of the Equation(31) and the definition of the Jacobi elliptic cosine function, we have</p><disp-formula id="scirp.43178-formula106937"><label>(32)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\26516e1d-5df1-4a65-b4d1-ce62072e0b37.png"  xlink:type="simple"/></disp-formula><p>The corresponding solutions is</p><disp-formula id="scirp.43178-formula106938"><label>(33)</label><graphic position="anchor" xlink:href="htmlimages\5-1720091x\77482f11-d0ef-46c9-a4eb-d51855acc8db.png"  xlink:type="simple"/></disp-formula><p>In Equations (17), (18), (19), (21), (26), (28) and (33), the integration constant <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\981c011e-4535-47a3-86d5-91dbe209b6eb.png" xlink:type="simple"/></inline-formula> has been rewritten,but we still use it. The solutions <inline-formula><inline-graphic xlink:href="tmlimages\5-1720091x\8cf141f2-eef5-4df4-8c5e-2d9a58e7566b.png" xlink:type="simple"/></inline-formula> are all possible exact traveling wave solutions to Equation (1). It is easy to write the corresponding solutions to the Benjamin Ono equation. For brevity, we omitted.</p></sec><sec id="s3"><title>3. Conclusion</title><p>Trial equation method is a systematic method to solve nonlinear differential equations. The advantage of this method is that we can deal with nonlinear equations with linear methods. This method has the characteristics of simple steps and clear effectivity. Based on the idea of the trial equation method and the aid of the computerized symbolic computation, some exact traveling wave solutions to the Benjamin Ono equation have been obtained. With the same method, some of other equations can be dealt with.</p></sec><sec id="s4"><title>Acknowledgements</title><p>I would like to thank the referees for their valuable suggestions.</p></sec><sec id="s5"><title>REFERENCES</title><p>[<xref ref-type="bibr" rid="scirp.43178-ref1">1</xref>]&#160;M. J. Ablowitz and P. A. Clarkson, “Solitous, Non-Linear Evolution Equations and Inverse Scattering,” Cambridge University Press, Cambridge, 1991.</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref2">2</xref>]&#160;R. Hirota, “Exact Envelope-Soliton Solutions of a Nonlinear Wave Equation,” Journal of Mathematical Physics, Vol. 14, 1973, p. 805. http://dx.doi.org/10.1063/1.1666399</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref3">3</xref>]&#160;R. Hirota and J. Satsuma, “Soliton Solutions of a Coupled Korteweg-de Vries Equation,” Physics Letters A, Vol. 85, No. 8-9, 1981, p. 407-408. http://dx.doi.org/10.1016/0375-9601(81)90423-0</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref4">4</xref>]&#160;E. Fan, “Extended Tank-Function Method and Its Applications to Nonlinear Equations,” Physics Letters A, Vol. 277, No. 4, 2000, pp. 212-218.</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref5">5</xref>]&#160;C. T. Yan, “A Simple Transformation for Nonlinear Waves,” Physics Letters A, Vol. 224, No. 1-4, 1996, pp. 77-84. http://dx.doi.org/10.1016/S0375-9601(96)00770-0</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref6">6</xref>]&#160;M. Wang, Y. Zhou and Z. Li, “Application of a Homogeneous Balance Method to Exact Solutions of Nonlinearequations in Mathematical Physics,” Physics Letters A, Vol. 216, No. 1, 1996, pp. 67-75.</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref7">7</xref>]&#160;M. L. Wang, “Solitary Wave Solutions for Variant Boussinesq Equations,” Physics Letters A, Vol. 199, No. 3-4, 1995, pp. 169-172. http://dx.doi.org/10.1016/0375-9601(95)00092-H</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref8">8</xref>]&#160;W. X. Ma and J. H. Lee, “A Transformed Rational Function Method and Exact Solutions to the 3 + 1 Dimensional Jimbo-Miwa Equation,” Chaos, Solitons and Fractals, Vol. 42, No. 3, pp. 1356-1363. http://dx.doi.org/10.1016/j.chaos.2009.03.043</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref9">9</xref>]&#160;C. S. Liu, “Trial Equation Method to Nonlinear Evolution Equations with Rank Inhomogenous: Mathematical Discussions and Its Applications,” Communications in Theoretical Physics, Vol. 45, No. 2, 2006, pp. 219-223. http://dx.doi.org/10.1088/0253-6102/45/2/005</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref10">10</xref>]&#160;C. S. Liu, “Trial Equation Method and its Applications to Nonlinear Evolution Equations,” Acta Physica Sinica, Vol. 54, No. 6, 2005, pp. 2505-2509.</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref11">11</xref>]&#160;C. S. Liu, “Using Trial Equation Method to Solve the Exact Solutions for two kinds of KdV Equations with Variable Coefficients,” Acta Physica Sinica, Vol. 54, No. 10, 2005, p. 4506.</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref12">12</xref>]&#160;C. S. Liu, “Representations and Classification of Traveling Wave Solutions to sinh-G&#246;rdon Equation,” Communications in Theoretical Physics, Vol. 49, No. 1, 2008, pp. 153-158.  http://dx.doi.org/10.1088/0253-6102/49/1/33</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref13">13</xref>]&#160;C. S. Liu, “Solution of ODE u'' + p(u)(u')<sup>2</sup><sup> </sup>+ q(u) = 0 and Applications to Classifications of All Single Travelling Wave Solutions to Some Nonlinear Mathematical Physics Equations,” Communications in Theoretical Physics, Vol. 49, No. 2, 2008, pp. 291-296. http://dx.doi.org/10.1088/0253-6102/49/2/07</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref14">14</xref>]&#160;C. S. Liu, “Applications of Complete Discrimination System for Polynomial for Classifications of Traveling Wave Solutions to Nonlinear Differential Equations,” Computer Physics Communications, Vol. 181, No. 2, 2010, pp. 317-324. http://dx.doi.org/10.1016/j.cpc.2009.10.006</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref15">15</xref>]&#160;C. S. Liu, “Classification of All Single Travelling Wave Solutions to Calogero-Degasperis-Focas Equation,” Communications in Theoretical Physics, Vol. 48, No. 10, 2007, pp. 601-604. http://dx.doi.org/10.1088/0253-6102/48/4/004</p><p>[<xref ref-type="bibr" rid="scirp.43178-ref16">16</xref>]&#160;C. S. Liu, “All Single Traveling Wave Solutions to Nizhnok-Novikov-Veselov Equation,” Communications in Theoretical Physics, Vol. 45, No. 6, 2006, pp. 991-992. http://dx.doi.org/10.1088/0253-6102/45/6/006</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.43178-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">M. J. Ablowitz and P. A. Clarkson, “Solitous, Non-Linear Evolution Equations and Inverse Scattering,” Cambridge University Press, Cambridge, 1991.</mixed-citation></ref><ref id="scirp.43178-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">R. Hirota, “Exact Envelope-Soliton Solutions of a Nonlinear Wave Equation,” Journal of Mathematical Physics, Vol. 14, 1973, p. 805. http://dx.doi.org/10.1063/1.1666399</mixed-citation></ref><ref id="scirp.43178-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">R. Hirota and J. Satsuma, “Soliton Solutions of a Coupled Korteweg-de Vries Equation,” Physics Letters A, Vol. 85, No. 8-9, 1981, p. 407-408. http://dx.doi.org/10.1016/0375-9601(81)90423-0</mixed-citation></ref><ref id="scirp.43178-ref4"><label>4</label><mixed-citation publication-type="other" xlink:type="simple">E. Fan, “Extended Tank-Function Method and Its Applications to Nonlinear Equations,” Physics Letters A, Vol. 277, No. 4, 2000, pp. 212-218.</mixed-citation></ref><ref id="scirp.43178-ref5"><label>5</label><mixed-citation publication-type="other" xlink:type="simple">C. T. Yan, “A Simple Transformation for Nonlinear Waves,” Physics Letters A, Vol. 224, No. 1-4, 1996, pp. 77-84. http://dx.doi.org/10.1016/S0375-9601(96)00770-0</mixed-citation></ref><ref id="scirp.43178-ref6"><label>6</label><mixed-citation publication-type="other" xlink:type="simple">M. Wang, Y. Zhou and Z. Li, “Application of a Homogeneous Balance Method to Exact Solutions of Nonlinearequations in Mathematical Physics,” Physics Letters A, Vol. 216, No. 1, 1996, pp. 67-75.</mixed-citation></ref><ref id="scirp.43178-ref7"><label>7</label><mixed-citation publication-type="other" xlink:type="simple">M. L. Wang, “Solitary Wave Solutions for Variant Boussinesq Equations,” Physics Letters A, Vol. 199, No. 3-4, 1995, pp. 169-172. http://dx.doi.org/10.1016/0375-9601(95)00092-H</mixed-citation></ref><ref id="scirp.43178-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">W. X. Ma and J. H. Lee, “A Transformed Rational Function Method and Exact Solutions to the 3 + 1 Dimensional Jimbo-Miwa Equation,” Chaos, Solitons and Fractals, Vol. 42, No. 3, pp. 1356-1363. http://dx.doi.org/10.1016/j.chaos.2009.03.043</mixed-citation></ref><ref id="scirp.43178-ref9"><label>9</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “Trial Equation Method to Nonlinear Evolution Equations with Rank Inhomogenous: Mathematical Discussions and Its Applications,” Communications in Theoretical Physics, Vol. 45, No. 2, 2006, pp. 219-223. http://dx.doi.org/10.1088/0253-6102/45/2/005</mixed-citation></ref><ref id="scirp.43178-ref10"><label>10</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “Trial Equation Method and its Applications to Nonlinear Evolution Equations,” Acta Physica Sinica, Vol. 54, No. 6, 2005, pp. 2505-2509.</mixed-citation></ref><ref id="scirp.43178-ref11"><label>11</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “Using Trial Equation Method to Solve the Exact Solutions for two kinds of KdV Equations with Variable Coefficients,” Acta Physica Sinica, Vol. 54, No. 10, 2005, p. 4506.</mixed-citation></ref><ref id="scirp.43178-ref12"><label>12</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “Representations and Classification of Traveling Wave Solutions to sinh-Gordon Equation,” Communications in Theoretical Physics, Vol. 49, No. 1, 2008, pp. 153-158. http://dx.doi.org/10.1088/0253-6102/49/1/33</mixed-citation></ref><ref id="scirp.43178-ref13"><label>13</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “Solution of ODE u'' + p(u)(u')2 + q(u) = 0 and Applications to Classifications of All Single Travelling Wave Solutions to Some Nonlinear Mathematical Physics Equations,” Communications in Theoretical Physics, Vol. 49, No. 2, 2008, pp. 291-296. http://dx.doi.org/10.1088/0253-6102/49/2/07</mixed-citation></ref><ref id="scirp.43178-ref14"><label>14</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “Applications of Complete Discrimination System for Polynomial for Classifications of Traveling Wave Solutions to Nonlinear Differential Equations,” Computer Physics Communications, Vol. 181, No. 2, 2010, pp. 317-324. http://dx.doi.org/10.1016/j.cpc.2009.10.006</mixed-citation></ref><ref id="scirp.43178-ref15"><label>15</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “Classification of All Single Travelling Wave Solutions to Calogero-Degasperis-Focas Equation,” Communications in Theoretical Physics, Vol. 48, No. 10, 2007, pp. 601-604. http://dx.doi.org/10.1088/0253-6102/48/4/004</mixed-citation></ref><ref id="scirp.43178-ref16"><label>16</label><mixed-citation publication-type="other" xlink:type="simple">C. S. Liu, “All Single Traveling Wave Solutions to Nizhnok-Novikov-Veselov Equation,” Communications in Theoretical Physics, Vol. 45, No. 6, 2006, pp. 991-992. http://dx.doi.org/10.1088/0253-6102/45/6/006</mixed-citation></ref></ref-list></back></article>