<?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">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2012.36079</article-id><article-id pub-id-type="publisher-id">AM-20078</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>
 
 
  New Explicit Solutions of the Generalized (2 + 1)-Dimensional Zakharov-Kuznetsov Equation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ang-Wei</surname><given-names>Wang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xi-Qiang</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ying-Yuan</surname><given-names>Zhang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Mathematics Sciences, Liaocheng University, Liaocheng, China</addr-line></aff><pub-date pub-type="epub"><day>21</day><month>06</month><year>2012</year></pub-date><volume>03</volume><issue>06</issue><fpage>523</fpage><lpage>527</lpage><history><date date-type="received"><day>March</day>	<month>28,</month>	<year>2012</year></date><date date-type="rev-recd"><day>April</day>	<month>28,</month>	<year>2012</year>	</date><date date-type="accepted"><day>May</day>	<month>5,</month>	<year>2012</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>
 
 
  his paper studies the generalized (2 + 1)-dimensional Zakharov-Kuznetsov equation using the (G'/G)-expand method, we obtain many new explicit solutions of the generalized (2 + 1)-dimensional Zakharov-Kuznetsov equation, which include hyperbolic function solutions, trigonometric function solutions and rational function solutions and so on.
 
</p></abstract><kwd-group><kwd>Zakharov-Kuznetsov Equation; The (G'/G)-Expand Method; Homogeneous Balance Principle; Explicit Solutions</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Nonlinear evolution equations in many areas play an important role. Thus solving nonlinear evolution equations (NLEEs) has become a valuable task. For this purpose, in the past few decades, due to availability of computer symbolic system like Mathematica or Maple, many significant methods have been developed, such as inverse scattering transformation (IST) [<xref ref-type="bibr" rid="scirp.20078-ref1">1</xref>], Jacobi elliptic function method [<xref ref-type="bibr" rid="scirp.20078-ref2">2</xref>], Hirota bilinear method [<xref ref-type="bibr" rid="scirp.20078-ref3">3</xref>], Sinecose function method [<xref ref-type="bibr" rid="scirp.20078-ref4">4</xref>], classic and non-classic Lie symmetry method [5-7], the Exp-function expansion method [<xref ref-type="bibr" rid="scirp.20078-ref8">8</xref>] and so on.</p><p>Recently, Wang [<xref ref-type="bibr" rid="scirp.20078-ref9">9</xref>] introduced a new method called the (G'/G)-expansion method to look for exact solutions of mathematical physics. Lot of studies have been conducted with NLEEs by using this method [10-12]. This method is direct, concise, elementary and effective, and can be used for NLEEs involving higher order nonlinear terms.</p><p>Let us consider the generalized (2 + 1)-dimensional ZK Equation with high-order nonlinear terms in the form as follows:</p><disp-formula id="scirp.20078-formula98668"><label>(1)</label><graphic position="anchor" xlink:href="4-7400787\8de58fbd-0d70-48a8-9c1e-5d0095bb9c30.jpg"  xlink:type="simple"/></disp-formula><p>where a, b, c and e are nonzero arbitrary constants and<img src="4-7400787\5a529354-4dc7-4024-8f08-335b94c3c8bb.jpg" />. When<img src="4-7400787\f6c56d26-a35f-4168-9dba-607cfcb2cedc.jpg" />, Equation (1) can be reduced to the standard (2 + 1)-dimensional ZK Equation. In 1974, Zakharov and Kuznetsov (ZK) [<xref ref-type="bibr" rid="scirp.20078-ref13">13</xref>] derived an equation which describes weakly nonlinear ion-acoustic waves in a strongly magnetized lossless plasma composed of coldions and hot isothermal electrons. The ZakhrovKuznetsov (ZK) Equation is also known as one of twodimensional generalizations of the KdV equation, another one being the Kadomtsev-Petviashvili (KP) Equation for example. The ZK Equation has been derived in the context of plasma physics [14,15]. Biswas and Zerrad [<xref ref-type="bibr" rid="scirp.20078-ref16">16</xref>] considered the ZK Equation with dual-power law nonlinearity and obtained 1-soliton solution by using the solitary wave ansatze. He [<xref ref-type="bibr" rid="scirp.20078-ref17">17</xref>] applied the homotopy perturbation method to the (2 + 1)-dimensional ZK Equation to search for traveling wave solutions. Using a subequation method (the elliptic equation is taken as a transformation), the traveling wave solutions for the (2 + 1) dimensional-ZK Equation are also studied by Fu [<xref ref-type="bibr" rid="scirp.20078-ref18">18</xref>]. I. Aslan has obtained solitary and periodic wave solutions [<xref ref-type="bibr" rid="scirp.20078-ref19">19</xref>].</p><p>In this paper, by use of the (G'/G)-expansion method to construct some new exact solutions of the generalized (2 + 1)-dimensional ZK Equation with nonlinear terms of any order.</p></sec><sec id="s2"><title>2. The (G'/G)-Expansion Method</title><p>Wang (Wang and Zhang, 2008) has summarized for using (G'/G)-expansion method:</p><p>Step 1: Combining the independent variables x and t into one variable<img src="4-7400787\a82fea72-fe58-419c-92ed-a6a8d015fe0c.jpg" />, we suppose that &#160; <img src="4-7400787\40f898f5-d29b-4a19-b8fb-f2fb373b37a1.jpg" />, which permits us reducing a partial differential equation (PDE)</p><disp-formula id="scirp.20078-formula98669"><label>(2.1)</label><graphic position="anchor" xlink:href="4-7400787\05faa837-76dd-4f47-b91c-8ece58a89237.jpg"  xlink:type="simple"/></disp-formula><p>to an ordinary differential equation (ODE) for <img src="4-7400787\3ed645a7-26ed-4699-92ae-12fb7ab18a82.jpg" /></p><disp-formula id="scirp.20078-formula98670"><label>(2.2)</label><graphic position="anchor" xlink:href="4-7400787\60705e1b-9a22-4bc1-b74e-e1eebcaed616.jpg"  xlink:type="simple"/></disp-formula><p>Step 2: Suppose that the solution of ODE (2.2) can be expressed by a polynomial in (G'/G) as follows:</p><disp-formula id="scirp.20078-formula98671"><label>(2.3)</label><graphic position="anchor" xlink:href="4-7400787\65d0c2b9-d5bf-44d4-82a6-cac7382e47e1.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-7400787\73658a4d-199f-446b-95e2-d0af072c8a2e.jpg" /> satisfies the second order LODE in the form</p><disp-formula id="scirp.20078-formula98672"><label>(2.4)</label><graphic position="anchor" xlink:href="4-7400787\62619be2-2c4f-42a9-8f9b-d0553e6bfc0f.jpg"  xlink:type="simple"/></disp-formula><p>the integer m can be determined by considering the homogeneous balance between the highest order derivatives and the nonlinear terms appearing in ODE (2.2).</p><p>Step 3: By substituting (2.3) into (2.2) and using the second order linear ODE (2.4), collecting all terms with the same order of (G'/G) together, the left-hand side of Equation (2.2) is converted into another polynomial in (G'/G). Equating each coefficient of this polynomial to zero yields a set of algebraic equations for <img src="4-7400787\ef386a8a-d5ed-4582-b085-4f298bc4efd3.jpg" />, <img src="4-7400787\1fa535ca-ef21-4f84-8800-532e44a0c07d.jpg" />, c and <img src="4-7400787\e0bb30e4-b950-4108-a2d8-d231acbfca1a.jpg" /> by using Maple, along with the general solutions of Equation (2.4) into (2.3), we can have more travelling wave solutions of the nonlinear evolution Equation (2.1).</p></sec><sec id="s3"><title>3. Exact Solutions of the Generalized (2 + 1)-Dimensional ZK Equation with Any-Order Nonlinear Terms</title><p>Firstly we take the form of the required solution as follows:</p><p><img src="4-7400787\bca9fd50-4411-4cda-b51a-7f7bf5664dcb.jpg" /><img src="4-7400787\e4c9d1ab-4332-46c7-a212-05ddd9bd2e7a.jpg" /> (3.1)</p><p>where k, l and m are constants to be determined later, Equation (1) becomes an ODE</p><disp-formula id="scirp.20078-formula98673"><label>(3.2)</label><graphic position="anchor" xlink:href="4-7400787\968e034a-c482-4d5e-87b9-e67af7e98043.jpg"  xlink:type="simple"/></disp-formula><p>Suppose that the solutions of (3.2) can be expressed by a polynomial in (G'/G) as follows:</p><disp-formula id="scirp.20078-formula98674"><label>(3.3)</label><graphic position="anchor" xlink:href="4-7400787\85ec3069-0ff7-4920-86f3-f20b06329aa9.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-7400787\fb8d67b5-95c5-4966-9efe-fdf8012ee1f1.jpg" /> satisfies the second order LODE in the form</p><disp-formula id="scirp.20078-formula98675"><label>(3.4)</label><graphic position="anchor" xlink:href="4-7400787\3194991e-159e-4459-912f-508b01c5ad81.jpg"  xlink:type="simple"/></disp-formula><p>the integer q can be determined by considering the homogeneous balance between the highest order derivatives and the nonlinear terms appearing in ODE (3.2).</p><p>Equation (3.4) can be changed into</p><disp-formula id="scirp.20078-formula98676"><label>(3.5)</label><graphic position="anchor" xlink:href="4-7400787\1f4070e1-3859-4416-ab70-a012e5364d89.jpg"  xlink:type="simple"/></disp-formula><p>By using Equation (3.5), by balancing the highest order partial derivative term and the nonlinear term in (3.2), we get the value of q,</p><p><img src="4-7400787\b7c3ca79-77c5-4348-90b5-7585e7a0341f.jpg" /></p><p>So<img src="4-7400787\39335917-cf80-4495-957b-d1ac4abd1c99.jpg" />, Thus we make transformation <img src="4-7400787\5d492358-dd2d-4926-bdbc-6a31507f5a5f.jpg" />and transform Equation (3.2) into the following ODE</p><disp-formula id="scirp.20078-formula98677"><label>(3.6)</label><graphic position="anchor" xlink:href="4-7400787\deeb7d31-7401-49a9-85f5-9fb7015cfe05.jpg"  xlink:type="simple"/></disp-formula><p>Suppose that the solutions of (3.6) can be expressed by a polynomial in (G'/G) as follows:</p><disp-formula id="scirp.20078-formula98678"><label>(3.7)</label><graphic position="anchor" xlink:href="4-7400787\0d06bf66-883b-4a9f-a86f-0a1e5f3bf0ee.jpg"  xlink:type="simple"/></disp-formula><p>By balancing the highest order partial derivative term and the nonlinear term in (3.6), we get the value of n = 2, thus we can write Equation (3.7) as</p><disp-formula id="scirp.20078-formula98679"><label>(3.8)</label><graphic position="anchor" xlink:href="4-7400787\cd3656fd-1e1c-4557-9912-057385f87eea.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="4-7400787\acc3aad2-2c8e-4bf8-8511-7c605b3da889.jpg" />, <img src="4-7400787\efdcd2fc-285b-4c2a-9b74-24dc4ab43c7a.jpg" />and <img src="4-7400787\00283fd4-5ed1-492d-9246-360ae96c1870.jpg" /> are constants to be determined.</p><p>With the help of the symbolic software Maple15, substitution of Equation (3.8) with Equation (3.4) into Equation (3.6), collecting the coefficients of (G'/G) and setting it to zero, so the set of algebraic equations possesses the following solutions Set 1.</p><p><img src="4-7400787\9006f57a-f0c4-4ffd-b0f0-8d8c2e268717.jpg" />,</p><p><img src="4-7400787\ff57893c-da9a-43a6-b269-924d35aa25e7.jpg" />,</p><p><img src="4-7400787\e6f592bb-62f2-4bc1-a0b2-0aea918845dc.jpg" /></p><p>Set 2.</p><p><img src="4-7400787\f61fc45c-9ba1-44ae-933e-e64b3c583acd.jpg" /></p><p><img src="4-7400787\2053c34e-1aa3-4586-b583-4b5374d9ca5a.jpg" />,</p><p><img src="4-7400787\a588bfab-f895-4a78-bc48-99d32eb9b1f5.jpg" /></p><p>Set 3.</p><p><img src="4-7400787\9db1ef2c-8ec6-4824-91d9-7eeecd8098f0.jpg" /></p><p><img src="4-7400787\bb654100-b2c9-41bf-b320-214d10b32b46.jpg" />,</p><p><img src="4-7400787\6e3736bf-d012-4312-b602-b4aa72b4d520.jpg" /></p><p>Therefore, substituting the general solutions of Equation (3.4) into (3.8), we can obtain that three types of travelling wave solutions of (3.6) as follows:</p><p>Case (Set 1).</p><p>When<img src="4-7400787\b1a24164-7e1a-41c5-8dc2-caedc5d42f1a.jpg" />, we obtain hyperbolic function solution</p><p><img src="4-7400787\7dc3199e-63d5-4270-830c-6b854883aac1.jpg" /></p><p>By using<img src="4-7400787\6e44da6c-ed2a-4f52-be85-e991c5cb22c6.jpg" />, the generalized (2 + 1)-dimensional ZK Equation with high-order nonlinear terms have the solution</p><p><img src="4-7400787\fca68b1e-73f0-4346-b893-89901442e3f3.jpg" /></p><p>If setting <img src="4-7400787\2a9ba346-92b5-41e6-a2d1-1caa94d4e586.jpg" /> then solution <img src="4-7400787\c55c0a2b-781d-4e8f-9329-c659839a2caf.jpg" /> becomes the wellknow kink-type solitary wave solution, namely</p><p><img src="4-7400787\36a36461-d37b-4f1e-946b-7884e7ec1ba5.jpg" /></p><p>When<img src="4-7400787\d8684cd5-9355-4ecb-9971-8f5b9e195bf4.jpg" />, we have trigonometric function solution</p><p><img src="4-7400787\0ef7c67c-0de2-4da8-9981-23fd74c9d15a.jpg" /></p><p>Similarly,</p><p><img src="4-7400787\c8718f50-5d64-48bd-b602-7c3a9c614d43.jpg" /></p><p>When<img src="4-7400787\8daa783e-05d7-4582-887f-f879af79bf2b.jpg" />, we have rational function solution</p><p><img src="4-7400787\44bb8f00-b79e-487a-a106-29795f0580de.jpg" /></p><p>So we can get</p><disp-formula id="scirp.20078-formula98680"><label>(3.9)</label><graphic position="anchor" xlink:href="4-7400787\cd2bbd98-188a-445b-a3ca-d10ed51efaa8.jpg"  xlink:type="simple"/></disp-formula><p>Case (Set 2).</p><p>When<img src="4-7400787\987aa77f-f075-4061-9f0e-7908d76b8947.jpg" />, we can obtain hyperbolic function solution</p><p><img src="4-7400787\781178ba-bdf1-4cbe-a941-ef39bea818cf.jpg" /></p><p>Similarly, by using<img src="4-7400787\f66710b7-24b6-4d55-b2b3-84e0391da32d.jpg" />, the generalized</p><p>(2 + 1)-dimensional ZK Equation with high-order nonlinear terms have the solution</p><p><img src="4-7400787\6d63d3cd-5cf4-4d17-ba48-0d9810a5f8b6.jpg" /></p><p>If setting <img src="4-7400787\675a1bcb-2283-4e20-b695-fbb25905e620.jpg" /> then solution <img src="4-7400787\1564c424-176e-49d8-938a-1eabde4e10d6.jpg" /> can be changed</p><p><img src="4-7400787\041196fe-0618-4263-aa6c-e2da849f7cd3.jpg" /></p><p>When<img src="4-7400787\35750305-e43c-4419-aa4a-de05e6ce47dc.jpg" />, we have trigonometric function solution</p><p><img src="4-7400787\7eebea8f-2158-41e4-ae44-416a3d32984a.jpg" /></p><p>Similarly,</p><p><img src="4-7400787\96079fcb-ceaf-424e-a993-aec06a53d9c2.jpg" />.</p><p>If setting<img src="4-7400787\880ec4ec-a7a8-4cd6-b8b3-7e90c4ed9383.jpg" />, one can get</p><p><img src="4-7400787\744e88f6-6c4e-4ae3-8634-f82a5a5a7b67.jpg" /></p><p>When<img src="4-7400787\9a638b90-59bb-46f5-8044-6347247fd346.jpg" />, we have rational function solution the same results as (3.9). where<img src="4-7400787\41e3fb07-befd-491b-977a-529aee305512.jpg" />, <img src="4-7400787\0578d933-6011-4212-ad38-e7d007532351.jpg" />and <img src="4-7400787\cfb18a2b-b79a-4aff-86b1-92ed219329bc.jpg" /> are arbitrary constants.</p><p>Case (Set 3).</p><p>When<img src="4-7400787\078622d8-17c5-46d5-b316-ed3cbd998ff9.jpg" />, we can get hyperbolic function solution</p><p><img src="4-7400787\938dd966-f781-450d-b6c0-3cff0c91684a.jpg" />.</p><p>By using<img src="4-7400787\8a771501-6017-4de9-8fce-e3ee91162df6.jpg" />, we can get the solution of Equation (1)</p><p><img src="4-7400787\dfa33a06-5e42-4e4a-852b-0d1f2f1a80a3.jpg" /></p><p>When<img src="4-7400787\877dba56-7b6b-4742-b9a6-15e48bab607f.jpg" />, one can get new trigonometric function solution</p><p><img src="4-7400787\606e760e-a9b2-4faa-bfa3-8fa888c9b46b.jpg" /></p><p>Therefore, we can have the new trigonometric function solution</p><p><img src="4-7400787\ae9b7bee-0751-4a58-9c17-b516bb98fa3d.jpg" /></p><p>When<img src="4-7400787\821a726e-2d3e-4b23-a127-3fad6bd54e9c.jpg" />, we can obtain rational function solution</p><p><img src="4-7400787\277dcedf-b3b9-4651-ad8c-2b4172b7bcd6.jpg" /></p><p>Thus</p><p><img src="4-7400787\efb91150-3495-47f8-98a0-0fe0456d951c.jpg" /></p><p>where</p><p><img src="4-7400787\73c2558a-8340-4900-a18a-d2774d61f1f1.jpg" />,</p><p><img src="4-7400787\ecf7941f-fc76-458e-9866-67098c42b56e.jpg" /><img src="4-7400787\24efac0b-78aa-4f70-a064-701c24deeaf0.jpg" />and <img src="4-7400787\5cbc3246-1566-4dba-9d33-31bea221772f.jpg" /> are arbitrary constants.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper (G'/G)-expansion method is used for constructing some new exact solutions for the generalized (2 + 1)-dimensional ZK Equation with high-order nonlinear terms arising in mathematical physics. And above all, we have successfully obtained some new exact solutions for the generalized (2 + 1)-dimensional ZK Equation with high-order nonlinear terms, which include hyperbolic function solutions, trigonometric function solutions and rational function solutions and so on. The physical relevance of the new solutions is clear for us. The performance of the method used here, is reliable and effective, and give more and new solutions. All of the solutions obtained in this paper have been verified with the help of Maple. The new type of explicit solutions might have impact on future researches.</p></sec><sec id="s5"><title>5. Acknowledgements</title><p>The project is supported by National Natural Science Foundation of China and China Academy of Engineering Physics (NSAF:11076015).</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.20078-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">M. J. Ablowitz and H. Segur, “Solitons and Inverse Scattering Transform,” SIAM, Philadelphia, 1981. 
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