<?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.2014.27074</article-id><article-id pub-id-type="publisher-id">JAMP-47033</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>Exact Solutions to the Generalized Benjamin Equation</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hua</surname><given-names>Gao</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Genhu</surname><given-names>Di</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Applied Mathematics, Yuncheng University, Yuncheng, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>gaohuaxx@126.com(HG)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>13</day><month>06</month><year>2014</year></pub-date><volume>02</volume><issue>07</issue><fpage>671</fpage><lpage>676</lpage><history><date date-type="received"><day>26</day>	<month>March</month>	<year>2014</year></date><date date-type="rev-recd"><day>26</day>	<month>April</month>	<year>2014</year>	</date><date date-type="accepted"><day>3</day>	<month>May</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>
	Based on the <disp-formula id="scirp.47033-formula2945"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/Edit_5f54e36b-32c7-435a-949f-23c9abeea8b7.bmp"/></disp-formula>-expansion method, a series of exact solutions of the
generalized Benjamin equation have been obtained. The travelling wave solutions
are expressed by the hyperbolic functions, the trigonometric functions and the
rational functions. It is shown that the <disp-formula id="scirp.47033-formula2946"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/Edit_dbd20090-2d67-482c-b32a-d47b55a438b9.bmp"/></disp-formula>-expansion method is concise, and its applications are
promising.
</p></abstract><kwd-group><kwd>Expansion Method</kwd><kwd> Generalized Benjamin Equation</kwd><kwd> Nonlinear Evolution Equations</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>It is well known that seeking exact solutions for nonlinear evolution equations (NLEES) plays an important role in mathematical physics. In the past five decades or so, many effective methods have been presented, which contain the inverse scattering method [<xref ref-type="bibr" rid="scirp.47033-ref1">1</xref>] , Hirota bilinear method [<xref ref-type="bibr" rid="scirp.47033-ref2">2</xref>] , the tanh-function method and its various extension [<xref ref-type="bibr" rid="scirp.47033-ref3">3</xref>] [<xref ref-type="bibr" rid="scirp.47033-ref4">4</xref>] , the sine-cosine function method [<xref ref-type="bibr" rid="scirp.47033-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.47033-ref6">6</xref>] , homogeneous balance method [<xref ref-type="bibr" rid="scirp.47033-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.47033-ref8">8</xref>] , Jacobi elliptic function method [<xref ref-type="bibr" rid="scirp.47033-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.47033-ref10">10</xref>] , the first-integral method [<xref ref-type="bibr" rid="scirp.47033-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.47033-ref12">12</xref>] , the sine-Gordon equation method [<xref ref-type="bibr" rid="scirp.47033-ref13">13</xref>] and the Exp-function method [<xref ref-type="bibr" rid="scirp.47033-ref14">14</xref>] -[<xref ref-type="bibr" rid="scirp.47033-ref16">16</xref>] .</p><p>Recently, Wang et al. [<xref ref-type="bibr" rid="scirp.47033-ref17">17</xref>] proposed a new method called the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\f6f45c96-f0eb-4c3d-ac0b-77b386f14d17.png" xlink:type="simple"/></inline-formula>-expansion method to look for travelling</p><p>wave solutions of nonlinear evolution equations (NLEEs). The <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\844dc598-4174-4869-9842-fc43a626934a.png" xlink:type="simple"/></inline-formula>-expansion method is based on the assump-</p><p>tions that the travelling wave solutions can be expressed by a polynomial in <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\5cca646b-8f1f-4917-95ef-67675104aead.png" xlink:type="simple"/></inline-formula> as follows:</p><disp-formula id="scirp.47033-formula2923"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\0ace2382-85d4-4495-bb50-f50c16d18dc7.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\1fbda69a-e2f4-4f04-96d0-ce84e2851bcd.png" xlink:type="simple"/></inline-formula> satisfies a second order linear ordinary differential equation (LODE):</p><disp-formula id="scirp.47033-formula2924"><label>(2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\6c33a7e8-7811-47be-a2c6-ca5ff366f265.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\35ab1781-ab38-480d-bfba-dd31c4ea8ccd.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\e37ac775-c67f-4637-b396-6424a5cb7da4.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\c0019055-08b0-4cf8-8698-1bf18e5880a0.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\8d270b37-c175-4ca6-8312-6fad845ba8d4.png" xlink:type="simple"/></inline-formula> is a constant. The degree of the polynomial can be de-</p><p>termined by considering the homogeneous balance between the highest order derivative and nonlinear terms ap- pearing in the given NLEE. The coefficients of the polynomial can be obtained by solving a set of algebraic eq-</p><p>uations resulted from the process of using the method. By using the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\86697723-4d1d-44bf-9f6e-818334e37be0.png" xlink:type="simple"/></inline-formula>-expansion method, many nonlinear</p><p>equations [<xref ref-type="bibr" rid="scirp.47033-ref17">17</xref>] -[<xref ref-type="bibr" rid="scirp.47033-ref27">27</xref>] have been successfully solved.</p><p>In the present paper, we will extend the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\8f8a827f-1821-4609-a83b-7bf7d71593ad.png" xlink:type="simple"/></inline-formula>-expansion method to the following generalized Benjamin equa-</p><p>tion:</p><disp-formula id="scirp.47033-formula2925"><label>(3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\a616cec8-a730-4f84-820f-485cd08b6049.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\dac48baa-8d69-4ab3-9b92-fe7639465b39.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\e1363bc5-0ee7-4f6e-adde-0e7a3b39eac7.png" xlink:type="simple"/></inline-formula> are constants. Equation (3) is used in the analysis of long wave in shallow water; see [<xref ref-type="bibr" rid="scirp.47033-ref28">28</xref>] . To the best of our knowledge, there are a few articles about this equation. Recently, by applying the extended tanh method, Taghizadeh et al. [<xref ref-type="bibr" rid="scirp.47033-ref29">29</xref>] obtained some exact solutions. In the subsequent section, we will illustrate</p><p>the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\aa682fbc-9f98-4a42-af2f-c1e13a49a1e7.png" xlink:type="simple"/></inline-formula>-expansion method in detail with the generalized Benjamin equation.</p></sec><sec id="s2"><title>2. Exact Solutions to the Generalized Benjamin Equation</title><p>First, in this section, we start out our study for Equation (3). Firstly, making the following wave variable</p><disp-formula id="scirp.47033-formula2926"><label>(4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\c504e3a4-cda3-408f-952a-4c67d84aa748.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\394b7d7f-98b9-4010-addc-b2f2cb6fcc01.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\1319d252-ddba-40c6-9c5f-f4abafaa7113.png" xlink:type="simple"/></inline-formula> are constants to be determined later, Equation (3) becomes the ODE</p><disp-formula id="scirp.47033-formula2927"><label>(5)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\a33f6088-9270-430a-9911-6787b48a3d3f.png"/></disp-formula><p>where the prime denotes the derivation with respect to<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\31eb4deb-9a60-4162-adcb-c3f20300f41b.png" xlink:type="simple"/></inline-formula>. Integrating Equation (5), twice and setting the con- stant of integrating to zero, we obtain</p><disp-formula id="scirp.47033-formula2928"><label>(6)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\abc52dc8-bb41-4589-bcc6-2a4342b23b26.png"/></disp-formula><p>Then, making the following transformation</p><disp-formula id="scirp.47033-formula2929"><label>(7)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\ed1dade3-bccf-429f-b4a0-f32cab5e0c57.png"/></disp-formula><p>We can obtain an equation for <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\07904374-c678-40bf-90b8-e12bef19a3c1.png" xlink:type="simple"/></inline-formula> as</p><disp-formula id="scirp.47033-formula2930"><label>(8)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\cca4ecd8-fe48-4d55-aa54-a4abfd729deb.png"/></disp-formula><p>Now, we make an ansatz (1) for the solution of Equation (8). Balancing the terms <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\91675f90-ea8f-45cf-b6b1-bac0e1c5a892.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\a1a9e42b-c90a-49dd-95eb-3eaecc4c57a1.png" xlink:type="simple"/></inline-formula> in Equation (8) yields the leading order<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\65d18940-0753-473f-b273-a4a72173b732.png" xlink:type="simple"/></inline-formula>. Therefore, we can write the solution of Equation (8) in the form</p><disp-formula id="scirp.47033-formula2931"><label>(9)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\2f440866-ca09-45db-8d27-bf7a94ba72c6.png"/></disp-formula><p>Substituting (2) and (9) into (8), collecting the coefficients of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\098b5bfc-a503-465d-ad08-e8e9c43cfedb.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\f7a04a22-fc55-467a-8e2d-b14f0cc8a380.png" xlink:type="simple"/></inline-formula> and set it to zero we ob-</p><p>tain the following system of algebraic equations for:<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\00bb029e-aef1-4a23-b9ca-89777d7a4b81.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\ee1b73a1-da4c-419f-82cd-6728d9c90e29.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\5c66d530-957c-4d46-b18c-0ac5429304fe.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\730df8f0-cd8a-4b7a-8622-ae76548f155e.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\3a3b8172-d9a2-47ba-9d80-6df2631bf080.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\07886e91-d247-4f3e-8504-fe4f57e01d58.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\2a9dd86e-3f66-420f-8ea3-a719b8394f2f.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.47033-formula2932"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\3988010f-d130-4b1c-ae42-baa51b9c3c05.png"/></disp-formula><p>Solving the above system by Matlab gives</p><disp-formula id="scirp.47033-formula2933"><label>(10)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\8e76e155-121d-4d0c-b187-ae0b793dc36f.png"/></disp-formula><disp-formula id="scirp.47033-formula2934"><label>(11)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\c51fbc68-2279-4263-a9e2-70c2a4cc0006.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\833393af-3bd6-4109-98ee-b995dda17d45.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\063663f9-f5b5-40cb-959b-889b6a0e8b17.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\92b94c60-7646-4d63-b41a-719002374905.png" xlink:type="simple"/></inline-formula> are arbitrary constants.</p><p>Substituting (10) (11) into (9) yields:</p><disp-formula id="scirp.47033-formula2935"><label>(12)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\36f07a5d-c4ae-4c9d-9f3c-b9b4117d8e67.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\2e275a4c-4fc3-4489-b83b-ed8ae99935aa.png" xlink:type="simple"/></inline-formula>.</p><p>Substituting the general solutions of Equation (2) into the formulae (12) we have three types of travelling wave solutions of the generalized Benjamin equation as follows:</p><p>When<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\61a724d1-15f5-4033-bb01-cb2b03e97ed9.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.47033-formula2936"><label>(13)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\c2eb7910-636f-4446-a95a-e14f4d1a50c5.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\9ef63060-5638-422e-86f7-0b98cc179bdc.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\0dfd2345-da18-408b-8e5a-46a3870d9bdb.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\bd676f59-8045-49c9-92c2-ad4958a991ab.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\046fc1d4-125b-4e51-8e60-9df8bf09df4c.png" xlink:type="simple"/></inline-formula> are arbitrary constants. It is</p><p>easy to see that the hyperbolic solution (13) can be rewritten at<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\6e18b17b-9432-4cce-af40-80209872da90.png" xlink:type="simple"/></inline-formula>, as follows</p><disp-formula id="scirp.47033-formula2937"><label>(14)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\452802e2-d5be-4ea7-9de3-f313dbd8cfd4.png"/></disp-formula><p>while at<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\2be567a9-51c4-409d-9b04-4d4ac1b8e437.png" xlink:type="simple"/></inline-formula>, one can obtain</p><disp-formula id="scirp.47033-formula2938"><label>(15)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\0ff84369-cd31-4a31-b811-1adad14f4a25.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\4c7a8fbb-fe7d-4a0f-9b69-6dbe4ee483e9.png" xlink:type="simple"/></inline-formula>.</p><p>When<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\d60fdf4e-2691-4ad9-8c95-8b5e6fc257d2.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.47033-formula2939"><label>(16)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\412bd726-f45f-4227-b6a7-c10e56287095.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\ac9f94ab-2f2a-4af6-bd36-f20afbe72dce.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\45d1296c-5e25-4965-a35c-c33f61ba48a7.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\2178361d-2f3b-4921-9478-f456866a18df.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\d2a02296-e67c-4fa8-b95a-04c3bbbd184e.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Simila-</p><p>rity, it is easy to see that the trigonometric solution (16) can be rewritten at <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\607754b8-20f7-4c3b-ab59-08b450876408.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\01d629a9-f466-4d9d-87ca-59d0853a6e1f.png" xlink:type="simple"/></inline-formula>, as follows</p><disp-formula id="scirp.47033-formula2940"><label>(17)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\393d27e6-081f-4bd1-a992-3b2fbfc5eba3.png"/></disp-formula><p>and</p><disp-formula id="scirp.47033-formula2941"><label>(18)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\fa531771-932e-4cf6-8567-5c68f3372acc.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\55a9f86a-0ef3-4efb-ae5c-7daaaefd83d8.png" xlink:type="simple"/></inline-formula>.</p><p>When<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\bb4107ad-1105-4c95-8412-4992f7cced94.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.47033-formula2942"><label>(19)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\3abcf5f6-14fc-4193-8957-201d9181bf97.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\badbe573-3bcb-43a5-a260-b0bb456f3732.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\c9bd1cfb-6d7a-46ba-b2bb-df91e53d4343.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\6a4d02e3-11ed-46c6-9dd9-ba0bb2efa78e.png" xlink:type="simple"/></inline-formula> are arbitrary constants.</p><p>Authors [<xref ref-type="bibr" rid="scirp.47033-ref29">29</xref>] have looked for exact solutions of Equation (3) using the wave variable<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\f646433e-8216-4915-98e0-64f1a2cbcf62.png" xlink:type="simple"/></inline-formula>, Equa- tion (3) should become the ODE</p><disp-formula id="scirp.47033-formula2943"><label>(20)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\78ce86a2-ea5f-40c6-afcd-7b51b6d6a2a0.png"/></disp-formula><p>not the ODE (7) in [<xref ref-type="bibr" rid="scirp.47033-ref29">29</xref>] in the following form</p><disp-formula id="scirp.47033-formula2944"><label>(21)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\7a0dc4e5-6247-4557-a8b9-68720419cebc.png"/></disp-formula><p>Therefore, the exact solutions given in [<xref ref-type="bibr" rid="scirp.47033-ref29">29</xref>] are wrong. To the best of our knowledge, solutions (13), (16) and (19) have not been reported in literature.</p></sec><sec id="s3"><title>3. Conclusion</title><p>The <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\cf96fdec-ee72-4704-8a51-86d8abbe2e60.png" xlink:type="simple"/></inline-formula>-expansion method has been successfully applied here to seek exact solutions of the generalized Ben-</p><p>jamin equation. As a result, a series of new exact solutions are obtained. The solution procedure is very simple and the travelling wave solutions are expressed by the hyperbolic functions, the trigonometric functions and the rational functions. To the best of our knowledge, these solutions have not been reported in literature. It is shown</p><p>that the <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\20-1720140x\c854f4a2-45c0-41fd-ad7f-e5bbf2b1d5d2.png" xlink:type="simple"/></inline-formula>-expansion method provides a very effective and powerful mathematical tool for solving nonlinear</p><p>equations in mathematical physics.</p></sec><sec id="s4"><title>Acknowledgements</title><p>This work was supported by the research project of Yuncheng University (No.YQ-2011013, YQ-2011068, XK- 2012004).</p></sec></body><back><ref-list><title>References</title><ref id="scirp.47033-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">ABLOWITZ, M.J. AND CLARKSON, P.A. (1991) SOLITONS, NONLINEAR EVOLUTION EQUATIONS AND INVERSE SCATTERING. CAMBRIDGE UNIVERSITY PRESS, NEW YORK. HTTP://DX.DOI.ORG/10.1017/CBO9780511623998</mixed-citation></ref><ref id="scirp.47033-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">HIROTA, R. 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