<?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.2015.312181</article-id><article-id pub-id-type="publisher-id">JAMP-61765</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>
 
 
  Analytical Treatment of the Evolutionary (1 + 1)-Dimensional Combined KdV-mKdV Equation via the Novel (G'/G)-Expansion Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>d.</surname><given-names>Nur Alam</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>Fethi</surname><given-names>Bin Muhammad Belgacem</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>M.</surname><given-names>Ali Akbar</given-names></name><xref ref-type="aff" rid="aff3"><sup>3</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Pabna University of Science &amp;amp; Technology, Pabna, Bangladesh</addr-line></aff><aff id="aff2"><addr-line>Department of Mathematics, Faculty of Basic Education, PAAET, Al-Ardhiya, Kuwait</addr-line></aff><aff id="aff3"><addr-line>Department of Applied Mathematics, University of Rajshahi, Rajshahi, Bangladesh</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>nuralam.pstu23@gmail.com(DNA)</email>;<email>fbmbelgacem@gmail.com(FBMB)</email>;<email>ali_math74@yahoo.com(MAA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>04</day><month>12</month><year>2015</year></pub-date><volume>03</volume><issue>12</issue><fpage>1571</fpage><lpage>1579</lpage><history><date date-type="received"><day>24</day>	<month>October</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>5</month>	<year>December</year>	</date><date date-type="accepted"><day>8</day>	<month>December</month>	<year>2015</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 novel (G'/G)-expansion method is a powerful and simple technique for finding exact traveling wave solutions to nonlinear evolution equations (NLEEs). In this article, we study explicit exact traveling wave solutions for the (1 + 1)-dimensional combined KdV-mKdV equation by using the novel (G'/G)-expansion method. Consequently, various traveling wave solutions patterns including solitary wave solutions, periodic solutions, and kinks are detected and exhibited.
 
</p></abstract><kwd-group><kwd>Novel (G'/G)-Expansion Method</kwd><kwd> (1 + 1)-Dimensional Combined KdV-mKdV Equation</kwd><kwd> Kink Patterns</kwd><kwd> Nonlinear Evolution Equation</kwd><kwd> Solitary Wave Solutions</kwd><kwd> Traveling Wave Solutions</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>NLEEs arise in a wide variety of disciplines physical problems such as in physics, biology, fluid mechanics, solid-state physics, biophysics, solid mechanics, condensed matter physics, plasma physics, quantum mechanics, optical fibers, elastic media, reaction-diffusion models, and quantum field theory. Recently, many kinds of powerful methods have been proposed to find exact traveling wave solutions of NLEEs e.g., the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x7.png" xlink:type="simple"/></inline-formula>- expansion [<xref ref-type="bibr" rid="scirp.61765-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.61765-ref3">3</xref>] , the (G'/G)-expansion method [<xref ref-type="bibr" rid="scirp.61765-ref4">4</xref>] -[<xref ref-type="bibr" rid="scirp.61765-ref7">7</xref>] , the wave translation method [<xref ref-type="bibr" rid="scirp.61765-ref8">8</xref>] , the Ansatz method [<xref ref-type="bibr" rid="scirp.61765-ref9">9</xref>] [<xref ref-type="bibr" rid="scirp.61765-ref10">10</xref>] , the Darboux transformation method [<xref ref-type="bibr" rid="scirp.61765-ref11">11</xref>] , the Hopf-Coletrans formation [<xref ref-type="bibr" rid="scirp.61765-ref12">12</xref>] , the Miura transformation [<xref ref-type="bibr" rid="scirp.61765-ref13">13</xref>] , the Jacobi elliptic function method [<xref ref-type="bibr" rid="scirp.61765-ref14">14</xref>] , the A domian decomposition method [<xref ref-type="bibr" rid="scirp.61765-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.61765-ref16">16</xref>] , the method of bifurcation of planar dynamical systems [<xref ref-type="bibr" rid="scirp.61765-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.61765-ref18">18</xref>] , the inverse scattering transform method [<xref ref-type="bibr" rid="scirp.61765-ref19">19</xref>] , the multiple- expansion method [<xref ref-type="bibr" rid="scirp.61765-ref20">20</xref>] , Homotopy analysis method [<xref ref-type="bibr" rid="scirp.61765-ref21">21</xref>] [<xref ref-type="bibr" rid="scirp.61765-ref22">22</xref>] , three-wave method [<xref ref-type="bibr" rid="scirp.61765-ref23">23</xref>] , extended homoclinic test approach [<xref ref-type="bibr" rid="scirp.61765-ref24">24</xref>] , the improved F-expansion method [<xref ref-type="bibr" rid="scirp.61765-ref25">25</xref>] , the projective Riccati equation method [<xref ref-type="bibr" rid="scirp.61765-ref26">26</xref>] , and the Weirstrass elliptic function method [<xref ref-type="bibr" rid="scirp.61765-ref27">27</xref>] to name a few. The novel (G'/G)-expansion method is beginning to find a pragmatic ever increasing use as can be seen in [<xref ref-type="bibr" rid="scirp.61765-ref28">28</xref>] -[<xref ref-type="bibr" rid="scirp.61765-ref33">33</xref>] . Worthy is it to note perhaps that rudiments of the (G'/G)-expansion method was used by Eckstein and Belgacem, as early as the late 80’s, to describe the platelet transport behavior in blood vessels, [<xref ref-type="bibr" rid="scirp.61765-ref34">34</xref>] -[<xref ref-type="bibr" rid="scirp.61765-ref36">36</xref>] . Recently, Alam and Belgacem in their study appearing in the Waves, Wavelets and Fractals-Abstract Analysis Journal, applied the novel method to the long wave equation, [<xref ref-type="bibr" rid="scirp.61765-ref37">37</xref>] . The aim of this paper is to find exact and solitary wave solutions of the (1 + 1)-dimensional combined KdV-mKdV equation by the novel (G'/G)-expansion method.</p></sec><sec id="s2"><title>2. Description of the Method</title><p>For a given nonlinear wave equation with one physical field <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x8.png" xlink:type="simple"/></inline-formula> in two variables x and t</p><disp-formula id="scirp.61765-formula307"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x9.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x10.png" xlink:type="simple"/></inline-formula> and P is a polynomial about u in and its derivatives.</p><p>Let us consider that the traveling wave variable is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x11.png" xlink:type="simple"/></inline-formula>,. (2)</p><p>The traveling wave variable (2), transforms (1) into a nonlinear ODE for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x13.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.61765-formula308"><label>. (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x14.png"  xlink:type="simple"/></disp-formula><p>We seek for the solution of Equation (3) in the following generalized ansatze</p><disp-formula id="scirp.61765-formula309"><label>, (4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x15.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.61765-formula310"><label>. (5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x16.png"  xlink:type="simple"/></disp-formula><p>Herein <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x17.png" xlink:type="simple"/></inline-formula> or α<sub>N</sub> might be zero, but both of them could not be zero simultaneously. α<sub>j</sub> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x18.png" xlink:type="simple"/></inline-formula> and d are constants to be determined later and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x19.png" xlink:type="simple"/></inline-formula> satisfies the second order nonlinear ODE:</p><disp-formula id="scirp.61765-formula311"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x20.png"  xlink:type="simple"/></disp-formula><p>where prime denotes the derivative with respect to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x21.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x22.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x23.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x24.png" xlink:type="simple"/></inline-formula>are real parameters.</p><p>The Cole-Hopf transformation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x25.png" xlink:type="simple"/></inline-formula> reduces Equation (6) into Riccati equation:</p><disp-formula id="scirp.61765-formula312"><label>. (7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x26.png"  xlink:type="simple"/></disp-formula><p>Equation (7) has individual twenty five solutions (see Zhu, [<xref ref-type="bibr" rid="scirp.61765-ref38">38</xref>] for details).</p><p>The value of the positive integer N can be determined by balancing the highest order linear terms with the nonlinear terms of the highest order come out in Equation (3). If the degree of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x27.png" xlink:type="simple"/></inline-formula> is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x28.png" xlink:type="simple"/></inline-formula>, then the degree of the other expressions will be as follows:</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x29.png" xlink:type="simple"/></inline-formula>.</p><p>Substituting Equation (4) including Equations (5) and (6) into Equation (3), we obtain polynomials in</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x30.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x31.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x32.png" xlink:type="simple"/></inline-formula>. Collecting all coefficients of identical power of the re-</p><p>sulted polynomials to zero, yields an over-determined set of algebraic equations for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x33.png" xlink:type="simple"/></inline-formula>, d and V.</p><p>Suppose the value of the constants can be obtained by solving the algebraic equations obtained in Step 4. Substituting the values of the constants together with the solutions of Equation (6), we will obtain some new and comprehensive exact traveling wave solutions to the nonlinear evolution Equation (1).</p></sec><sec id="s3"><title>3. The (1 + 1)-Dimensional Combined KdV-mKdV Equation</title><p>In this section, we will employ the novel (G'/G)-expansion method to get several novel and further wide-ranging exact traveling wave solutions to the famous (1 + 1)-dimensional combined KdV-mKdV equation.</p><p>Let us consider the (1 + 1)-dimensional combined KdV-mKdV equation</p><disp-formula id="scirp.61765-formula313"><label>. (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x34.png"  xlink:type="simple"/></disp-formula><p>Using the traveling wave transformation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x35.png" xlink:type="simple"/></inline-formula>, Equation (8) is converted into the following ODE:</p><disp-formula id="scirp.61765-formula314"><label>. (9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x36.png"  xlink:type="simple"/></disp-formula><p>Integrating Equation (9), we obtain</p><disp-formula id="scirp.61765-formula315"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x37.png"  xlink:type="simple"/></disp-formula><p>where C is a constant of integration. Inserting Equation (4) into Equation (10) and balancing the highest order derivative <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x38.png" xlink:type="simple"/></inline-formula> with the nonlinear term of the highest order<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x39.png" xlink:type="simple"/></inline-formula>, we obtain<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x40.png" xlink:type="simple"/></inline-formula>.</p><p>Therefore, the solution of Equation (10) takes the form,</p><disp-formula id="scirp.61765-formula316"><label>. (11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x41.png"  xlink:type="simple"/></disp-formula><p>Substituting Equation (11) into Equation (10), the left hand side is transformed into polynomials of</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x42.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x43.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x44.png" xlink:type="simple"/></inline-formula>. Equating the coefficients of like power of these poly-</p><p>nomials to zero, we obtain an over-determine set of algebraic equations (for simplicity we leave out to display the equations) for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x45.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x46.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x47.png" xlink:type="simple"/></inline-formula>, d, C and V. Solving the over-determined set of algebraic equations by using the symbolic computation software, such as Maple 13, we obtain</p><disp-formula id="scirp.61765-formula317"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x48.png"  xlink:type="simple"/></disp-formula><p>where d, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x49.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x50.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x51.png" xlink:type="simple"/></inline-formula> are arbitrary constants.</p><p>For Set, substituting Equation (12) and the values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x52.png" xlink:type="simple"/></inline-formula> into Equation (11) and simplifying, we obtain the following:</p><p>When <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x53.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x54.png" xlink:type="simple"/></inline-formula> (or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x55.png" xlink:type="simple"/></inline-formula>),</p><disp-formula id="scirp.61765-formula318"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x56.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x57.png" xlink:type="simple"/></inline-formula>, and d, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x58.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x59.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x60.png" xlink:type="simple"/></inline-formula> are arbitrary constants.</p><disp-formula id="scirp.61765-formula319"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x61.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula320"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x62.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula321"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x63.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula322"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x64.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula323"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x65.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula324"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x66.png"  xlink:type="simple"/></disp-formula><p>where A and B are real constants.</p><disp-formula id="scirp.61765-formula325"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x67.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula326"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x68.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula327"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x69.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula328"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x70.png"  xlink:type="simple"/></disp-formula><p>When <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x71.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x72.png" xlink:type="simple"/></inline-formula> (or<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x73.png" xlink:type="simple"/></inline-formula>),</p><disp-formula id="scirp.61765-formula329"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x74.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula330"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula331"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula332"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula333"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x78.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula334"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x79.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula335"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x80.png"  xlink:type="simple"/></disp-formula><p>where A and B are arbitrary constants such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x81.png" xlink:type="simple"/></inline-formula>.</p><disp-formula id="scirp.61765-formula336"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x82.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula337"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x83.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula338"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x84.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula339"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x85.png"  xlink:type="simple"/></disp-formula><p>When <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x86.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x87.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.61765-formula340"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x88.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.61765-formula341"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x89.png"  xlink:type="simple"/></disp-formula><p>where k is an arbitrary constant.</p><p>When <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x90.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x91.png" xlink:type="simple"/></inline-formula>, the solution of Equation (8) is,</p><disp-formula id="scirp.61765-formula342"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-1720412x92.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-1720412x93.png" xlink:type="simple"/></inline-formula> is an arbitrary constant.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In this letter, the novel (G'/G)-expansion method has been successfully applied to find the exact solution for the (1 + 1)-dimensional combined KdV-mKdV equation. The novel (G'/G)-expansion method is used to find a new exact traveling wave solution. The results show that the novel (G'/G)-expansion method is reliable and effective tool to solve the (1 + 1)-dimensional combined KdV-mKdV equation. Thus the novel (G'/G)-expansion method could be a powerful mathematical tool for solving NLEEs.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The Authors offer sincere thanks to the referees and editorial board of JAMP for their helpful and kind support. Furthermore, Fethi Bin Muhammad Belgacem is pleased to acknowledge the continued support of the Public Authority for Applied Education and Training (PAAET RD) for their continued support.</p></sec><sec id="s6"><title>Cite this paper</title><p>Md. NurAlam,Fethi Bin MuhammadBelgacem,M. AliAkbar, (2015) Analytical Treatment of the Evolutionary (1 + 1)-Dimensional Combined KdV-mKdV Equation via the Novel (G'/G)-Expansion Method. Journal of Applied Mathematics and Physics,03,1571-1579. doi: 10.4236/jamp.2015.312181</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.61765-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Hafez, M.G., Alam, Md.N. and Akbar, M.A. (2015) Traveling Wave Solutions for Some Important Coupled Nonlinear Physical Models via the Coupled Higgs Equation and the Maccari System. Journal of King Saud University—Science, 27, 105-112. http://dx.doi.org/10.1016/j.jksus.2014.09.001</mixed-citation></ref><ref id="scirp.61765-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Alam, Md.N., Hafez, M.G., Akbar, M.A. and Roshid, H.O. 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