<?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.2014.27070</article-id><article-id pub-id-type="publisher-id">JAMP-47023</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>The Periodic Solitary Wave Solutions for the (2 + 1)-Dimensional Fifth-Order KdV Equation</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Xianghua</surname><given-names>Meng</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>School of Applied Science, Beijing Information Science and Technology University, Beijing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>xhmeng@bistu.edu.cn</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>639</fpage><lpage>643</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>
	The (2 + 1)-dimensional fifth-order KdV equation is an important higher-dimensional
and higher-order extension of the famous KdV equation in fluid dynamics. In this
paper, by constructing new test functions, we investigate the periodic solitary
wave solutions for the (2 + 1)-dimensional fifth-order KdV equation by virtue of
the Hirota bilinear form. Several novel analytic solutions for such a model are
obtained and verified with the help of symbolic computation.
</p></abstract><kwd-group><kwd>(2 + 1)-Dimensional Fifth-Order KdV Equation</kwd><kwd> Periodic Solitary Wave Solutions</kwd><kwd> Hirota Bilinear Form</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The soliton equations play a very important role in the study of nonlinear phenomena in different fields such as the fluid physics, nonlinear optics, plasma physics and so on [<xref ref-type="bibr" rid="scirp.47023-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.47023-ref2">2</xref>] . The researches on the explicit analytic solutions for the soliton equations can help understand the nonlinear dynamics better. With the development of soliton theory, there are many systematic approaches solving different kinds of soliton solutions, such as the in- verse scattering transformation [<xref ref-type="bibr" rid="scirp.47023-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.47023-ref2">2</xref>] , the Darboux transformation [<xref ref-type="bibr" rid="scirp.47023-ref3">3</xref>] , the variable seperation method [<xref ref-type="bibr" rid="scirp.47023-ref4">4</xref>] , the bilinear method and so on [<xref ref-type="bibr" rid="scirp.47023-ref5">5</xref>] -[<xref ref-type="bibr" rid="scirp.47023-ref7">7</xref>] . Among those methods, the bilinear method is a powerful and direct approach to find soliton solutions for the nonlinear partial differential equations. Besides the soliton solutions, Dai has presented that the periodic solitary wave solutions for the soliton equations can be obtained by suitable test functions using the bilinear form [<xref ref-type="bibr" rid="scirp.47023-ref8">8</xref>] .</p><p>In this paper, we will consider the (2 + 1)-dimensional fifth-order KdV equation</p><disp-formula id="scirp.47023-formula2800"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\cda9e08c-9a09-41a5-b358-0cf081cb7eb6.png"/></disp-formula><p>with<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\2f376834-3454-410b-97d3-810bf5e7bcae.png" xlink:type="simple"/></inline-formula>, which is a (2 + 1)-dimensional analogue of the Caudrey-Dodd-Gibbon-Kotera-Sawada (CDGKS) equation [<xref ref-type="bibr" rid="scirp.47023-ref9">9</xref>] . When<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\3c537ab0-7bdd-44bf-9d7f-65fadec5acf9.png" xlink:type="simple"/></inline-formula>, it can be reduced to the CDGKS equation. Equation (1) was first pro- posed by Konopelchenko and Dubovsky [<xref ref-type="bibr" rid="scirp.47023-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.47023-ref11">11</xref>] . In Ref. [<xref ref-type="bibr" rid="scirp.47023-ref12">12</xref>] , the quasi-periodic solutions for Equation (1) have been obtained in terms of the Riemann theta functions. The symmetry transformations for Equation (1) have been given based on its Lax pair [<xref ref-type="bibr" rid="scirp.47023-ref13">13</xref>] . In this paper, with the help of symbolic computation, some novel pe- riodic solitary wave solutions for Equation (1) will be derived based on the bilinear form.</p></sec><sec id="s2"><title>2. Bilinear Form</title><p>According to the leading order analysis in the Painlev&#233; test, we can find the dependent variable transformation for Equation (1),</p><disp-formula id="scirp.47023-formula2801"><label>, (2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\08a42ed3-7751-4505-83b6-c9fb95debd68.png"/></disp-formula><p>with<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\21b802bd-16fc-4fb5-af03-e5b0bf8ba140.png" xlink:type="simple"/></inline-formula>. Substituting Transformation (2) into Equation (1), the following bilinear form can be ob- tained,</p><disp-formula id="scirp.47023-formula2802"><label>, (3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\31aa64e7-0dd2-4256-b03e-ac1f83ea0c97.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\96a76e86-bc07-4905-910c-99e3c34c182d.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\90c70f97-2bd8-492d-886e-6dcd30d52925.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\782a6ebb-cfe6-4159-a4a9-27613d8c34c2.png" xlink:type="simple"/></inline-formula> are the bilinear derivative operators [<xref ref-type="bibr" rid="scirp.47023-ref14">14</xref>] defined as,</p><disp-formula id="scirp.47023-formula2803"><label>.</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\af8b5faf-78b3-4d1b-b8db-4a61e5c18ddf.png"/></disp-formula></sec><sec id="s3"><title>3. Periodic Solitary Wave Solutions</title><p>In this section, according to different test functions for<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\dc792c57-3734-4bc7-b827-ac0a39efccee.png" xlink:type="simple"/></inline-formula>, we will derive the periodic solitary wave solutions for Equation (1).</p><sec id="s3_1"><title>3.1. Single Periodic Solitary Wave Solutions</title><p>Taking <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\6eddd228-985a-4eec-a5b9-56c956ff6547.png" xlink:type="simple"/></inline-formula> in Equation (3) as the following form</p><disp-formula id="scirp.47023-formula2804"><label>. (4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\7c675202-2c03-409a-8386-c0a2143c15d4.png"/></disp-formula><p>Substituting Solution (4) into the bilinearized equation (3), and equating the coefficients of different tri- angle and exponential functions to be zero, we can obtain the following equations,</p><disp-formula id="scirp.47023-formula2805"><label>, (5)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\89f1ed9a-001b-48e6-8634-e59202f25c0e.png"/></disp-formula><disp-formula id="scirp.47023-formula2806"><label>, (6)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\1645641e-b2a8-4368-9348-3bda378fcc83.png"/></disp-formula><disp-formula id="scirp.47023-formula2807"><label>, (7)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\72760a21-3b17-4447-aa71-d2d1aa6ce249.png"/></disp-formula><disp-formula id="scirp.47023-formula2808"><label>, (8)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\ab7840bb-cb03-4ed4-83b5-42ee6ca298ee.png"/></disp-formula><disp-formula id="scirp.47023-formula2809"><label>, (9)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\7e8560bd-5d1c-4d36-8e2c-403604cb87d1.png"/></disp-formula><disp-formula id="scirp.47023-formula2810"><label>, (10)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\c08b5aa1-a5de-47a9-bf4d-06904b95a698.png"/></disp-formula><disp-formula id="scirp.47023-formula2811"><label>(11)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\b97ac43e-40ba-4401-b2c0-8a7d710cd9fe.png"/></disp-formula><p>Solving the above system, two sets of single periodic solitary wave solutions can be got.</p><p>Case 1:<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\08066bb0-c1e6-41cb-a8b4-c24e3cce1a49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\660e3437-e83e-40ce-a888-a02c5de34b2d.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\47ca1f0b-acc2-48c8-8bd9-4c9d631bf9b6.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\f3d3ae04-7e92-45a0-94ad-d7ecbb4f9de5.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\f33f4d64-7b75-4acb-bccb-0e47b07618a6.png" xlink:type="simple"/></inline-formula></p><p>Denoting</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\9b7b3c37-9d9a-44d0-b858-0ccaac948ff3.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\05f27084-0385-4f86-a2e5-8a6e6d4d515e.png" xlink:type="simple"/></inline-formula>,</p><p>then</p><disp-formula id="scirp.47023-formula2812"><label>. (12)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\ce27adec-7f20-4ea0-995a-af8b2f1f6069.png"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\c061890e-3f07-42cf-ba8c-6dc944fc410a.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\4454aa13-e592-476f-8f2c-2c7921f9fbf8.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Substituting <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\75ea314f-28fe-496d-b8aa-b366692d7581.png" xlink:type="simple"/></inline-formula> into the transformation (2), we can obtain the single periodic solitary wave solution</p><disp-formula id="scirp.47023-formula2813"><label>. (13)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\2b30cdc0-8e02-4214-b338-bf68cc328c8f.png"/></disp-formula><p>Case 2:<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\a5ba6786-1ccb-448a-b7e2-72c16292ff24.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\69fc0bf1-e74d-4221-b78b-bcc7d940a0c7.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\fdd0ed1c-9475-4d19-b041-c371d61d4b28.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\a0c5b2ef-5f3c-4d7c-97ec-d7a8d2ef3add.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\d6e25d34-7aff-4268-a876-5c775a536751.png" xlink:type="simple"/></inline-formula></p><p>Denoting</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\4a45f830-1956-4eed-9bfb-eb80c7b0335b.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\99c6a729-536c-4817-b73a-ef243934a7b6.png" xlink:type="simple"/></inline-formula>,</p><p>then</p><disp-formula id="scirp.47023-formula2814"><label>, (14)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\ae3b49ae-9f81-438f-ae79-734724da2bdb.png"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\1933194f-6f53-46ed-8521-cdb8802b8481.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\f41c58f9-ce4d-47be-844e-6740922f44c3.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Substituting <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\35b5310c-e736-47b2-8a2e-499403f553b0.png" xlink:type="simple"/></inline-formula> into the transformation (2), the following single periodic solitary wave solution can be obtained,</p><disp-formula id="scirp.47023-formula2815"><label>. (15)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\38389ffe-5965-42a7-b720-d9f0653dcf71.png"/></disp-formula></sec><sec id="s3_2"><title>3.2. Two Periodic Solitary Wave Solutions</title><p>Taking <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\cb1e6cd5-b9f9-42e4-9694-ea7802782552.png" xlink:type="simple"/></inline-formula> as the following form</p><disp-formula id="scirp.47023-formula2816"><label>. (16)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\72a01010-8d6a-4e51-ac8b-0110f664b3a7.png"/></disp-formula><p>Substituting <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\6bb9be08-e437-49aa-95f7-c92be0d1dd85.png" xlink:type="simple"/></inline-formula> into the bilinearized equation (3), and equating the coefficients of different triangle and ex- ponential functions to be zero, we can obtain the following equations,</p><disp-formula id="scirp.47023-formula2817"><label>,</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\641f1315-5c0c-4c12-aa22-aede99308b39.png"/></disp-formula><disp-formula id="scirp.47023-formula2818"><label>,</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\93020553-95aa-4ece-904b-17f0c6607acc.png"/></disp-formula><disp-formula id="scirp.47023-formula2819"><label>,</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\e3cf54a5-0630-4fe0-bcd5-3ebb0142e047.png"/></disp-formula><disp-formula id="scirp.47023-formula2820"><label>,</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\7155ee71-32ac-40a8-8b6c-da1e9125b6c2.png"/></disp-formula><disp-formula id="scirp.47023-formula2821"><label>,</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\8682863f-5835-42d9-b17c-6518c8129e7e.png"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\bd86db82-39c7-4f06-9de8-345318f1792f.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\3a338f33-c60d-4f4a-9e9b-df362de03119.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.47023-formula2822"><label>.</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\b19879bf-1024-49ed-b3af-364b35e19ee0.png"/></disp-formula><p>Solving the above equations, we can obtain some novel two periodic solitary solutions of Equation (1).</p><p>Case 1: <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\14b130ba-00d9-47f8-831f-ffb2aee19fc7.png" xlink:type="simple"/></inline-formula></p><p>Denoting</p><disp-formula id="scirp.47023-formula2823"><label>, (17)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\d259b6e3-df5d-49c2-8550-8ddcae7c6e0f.png"/></disp-formula><p>then</p><disp-formula id="scirp.47023-formula2824"><label>, (18)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\42b721ce-68ab-40e3-9d9c-51a671b299d7.png"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\ae821149-6bf6-447c-b6ce-712fdb4ac654.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Substituting <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\bee7d74e-1987-4aba-99e7-4bacd7db246c.png" xlink:type="simple"/></inline-formula> into the transformation (2), we can obtain the two periodic solitary wave solution</p><disp-formula id="scirp.47023-formula2825"><label>. (19)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\b3c7ae89-b3e6-442f-b7e3-1b144d762033.png"/></disp-formula><p>Case 2:<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\6adabddf-50a1-4d54-ac45-f396f0177b87.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\4d9770bf-1d65-4fc1-900a-8c8accd59ebc.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\c4d79071-bdbf-4295-a8f1-f14b95ecf3aa.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\333cb427-d400-4f9a-b546-612fe20da6de.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\ca851993-3e2a-4fd4-b767-66d42f49b642.png" xlink:type="simple"/></inline-formula></p><p>Denoting</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\e236d951-b8fc-48a3-8892-8e32e30621a9.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\3557d58c-2e16-4866-bc96-cc11796f9241.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\fd099778-f77a-4757-afc9-45fb539e280d.png" xlink:type="simple"/></inline-formula>,</p><p>then</p><disp-formula id="scirp.47023-formula2826"><label>. (20)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\34c79d45-4f22-4df6-8f43-c3d8238c7374.png"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\18bc6977-784d-4534-9cf5-ee17692555a7.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Substituting <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\43eaf882-92a4-4272-89ed-22b970a9568d.png" xlink:type="simple"/></inline-formula> into the transformation (2), we can obtain the two periodic solitary wave solution</p><disp-formula id="scirp.47023-formula2827"><label>. (21)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\ff137ad7-a428-4479-822e-8196e66ccab1.png"/></disp-formula><p>Case 3:<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\ca5d79dc-3f91-4aef-8ab9-ac38fa339ded.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\56b38937-7ef9-48df-a145-2b1c4522a4fc.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\9ceff0e1-2d50-4236-bad0-83946e926b15.png" xlink:type="simple"/></inline-formula>,</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\4596b995-4025-4b2d-a7a7-8c3f958ff771.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\4d996363-bb12-48be-9d5b-58cc5e70fc53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\571bb722-31a2-4374-80e2-26cff9770e0c.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\5593cf1a-a3bd-4d2f-8a6c-f8754129f70f.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.47023-formula2828"><label>,</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\1daa087f-6afc-44b9-9a72-b76670d4d61c.png"/></disp-formula><p>which can give two sets of solution. Denoting</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\9244810a-0a3c-47bb-9a92-1dbf69f3a232.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\7a228767-972f-4142-b2b6-d2e346b68d70.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\470f996e-20f8-4054-a1ca-c8a01008a577.png" xlink:type="simple"/></inline-formula>.</p><p>Then <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\11ae7773-793b-4ec7-b205-4c65f7375713.png" xlink:type="simple"/></inline-formula> can be obtained in the following form,</p><disp-formula id="scirp.47023-formula2829"><label>, (22)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\16-1720136x\a1478e73-8050-4315-a325-f047a684fa06.png"/></disp-formula><p>According to Transformation (2), we can yield another two periodic solitary wave solutions for Equation (1).</p></sec></sec><sec id="s4"><title>4. Conclusion</title><p>As the important (2 + 1)-dimensional higher-order generalization of the KdV equation, the solutions for the (2 + 1)-dimensional fifth-order KdV equation are good at understanding the nonlinear phenomena in the fluid dy- namics. In this paper, the bilinear form for such an equation is derived based on a logarithm transformation. And then, by choosing two kinds of test functions, we have derived six new sets of periodic solitary wave solutions and verified them using the symbolic computation. It is hoped that the results obtained in this paper can be of help for the study of (2 + 1)-dimensional fifth-order KdV equation and the potential real application.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This work has been supported by Beijing Excellent Talent Training Project (2013D005007000003), the Scien- tific Research Project of Beijing Educational Committee (No. SQKM201211232016) and the National Natural Science Foundation of China under Grant No. 61072145.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.47023-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.47023-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">OSBORNE, A.R. 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