<?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">IJMNTA</journal-id><journal-title-group><journal-title>International Journal of Modern Nonlinear Theory and Application</journal-title></journal-title-group><issn pub-type="epub">2167-9479</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ijmnta.2015.41004</article-id><article-id pub-id-type="publisher-id">IJMNTA-54539</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The exp(-&amp;phi;(&amp;xi;))-Expansion Method and Its Application for Solving Nonlinear Evolution Equations
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ahmoud</surname><given-names>A. E. Abdelrahman</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>Emad</surname><given-names>H. M. Zahran</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mostafa</surname><given-names>M. A. Khater</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Mathematical and Physical Engineering, College of Engineering Shubra, Benha University, Egypt</addr-line></aff><aff id="aff1"><addr-line>Department of Mathematics, Faculty of Science, Mansoura University, Mansoura, Egypt</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>mostafa.khater2024@yahoo.com(MMAK)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>16</day><month>02</month><year>2015</year></pub-date><volume>04</volume><issue>01</issue><fpage>37</fpage><lpage>47</lpage><history><date date-type="received"><day>15</day>	<month>February</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>6</month>	<year>March</year>	</date><date date-type="accepted"><day>11</day>	<month>March</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 exp(-φ(ξ))
  
  -expansion method is used as the first time to investigate the wave solution of a nonlinear dynamical system in a new double-Chain model of DNA and a diffusive predator-prey system. The proposed method also can be used for many other nonlinear evolution equations.
 
</p></abstract><kwd-group><kwd>Dynamical System in a New Double-Chain Model of DNA</kwd><kwd> A  Diffusive Predator-Prey System</kwd><kwd> Traveling Wave Solutions</kwd><kwd> Solitary Wave Solutions</kwd><kwd> Kink-Anti Kink Shaped</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The nonlinear partial differential equations of mathematical physics are major subjects in physical science [<xref ref-type="bibr" rid="scirp.54539-ref1">1</xref>] . Exact solutions for these equations play an important role in many phenomena in physics such as uid mechanics, hydrodynamics, optics, plasma physics and so on. Recently many new approaches for finding these solutions have been proposed, for example, extended Jacobian Elliptic Function Expansion Method [<xref ref-type="bibr" rid="scirp.54539-ref2">2</xref>] , the modified simple equation method [<xref ref-type="bibr" rid="scirp.54539-ref3">3</xref>] , the tanh method [<xref ref-type="bibr" rid="scirp.54539-ref4">4</xref>] , extended tended tanh-method [<xref ref-type="bibr" rid="scirp.54539-ref5">5</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref7">7</xref>] , sine-cosine method [<xref ref-type="bibr" rid="scirp.54539-ref8">8</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref10">10</xref>] , homogeneous balance method [<xref ref-type="bibr" rid="scirp.54539-ref11">11</xref>] [<xref ref-type="bibr" rid="scirp.54539-ref12">12</xref>] , F-expansion method [<xref ref-type="bibr" rid="scirp.54539-ref13">13</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref15">15</xref>] , exp-function method [<xref ref-type="bibr" rid="scirp.54539-ref16">16</xref>] [<xref ref-type="bibr" rid="scirp.54539-ref17">17</xref>] ,</p><p>trigonometric function series method [<xref ref-type="bibr" rid="scirp.54539-ref18">18</xref>] , <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x9.png" xlink:type="simple"/></inline-formula>-expansion method [<xref ref-type="bibr" rid="scirp.54539-ref19">19</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref22">22</xref>] , Jacobi elliptic function method [<xref ref-type="bibr" rid="scirp.54539-ref23">23</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref26">26</xref>] , the exp<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x10.png" xlink:type="simple"/></inline-formula>-expansion method [<xref ref-type="bibr" rid="scirp.54539-ref27">27</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref29">29</xref>] and so on.</p><p>The objective of this article is to apply the exp<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x11.png" xlink:type="simple"/></inline-formula>-expansion method for finding the exact traveling</p><p>wave solution of dynamical system in a new double-Chain model of DNA and a diffusive predator-prey system which play an important role in biology and mathematical physics.</p><p>The rest of this paper is organized as follows: In Section 2, we give the description of the exp<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x12.png" xlink:type="simple"/></inline-formula>-ex-</p><p>pansion method. In Section 3, we use this method to find the exact solutions of the nonlinear evolution equations pointed out above. In Section 4, conclusions are given.</p></sec><sec id="s2"><title>2. Description of Method</title><p>Consider the following nonlinear evolution equation</p><disp-formula id="scirp.54539-formula41"><label>(2.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x13.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x14.png" xlink:type="simple"/></inline-formula> is a polynomial in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x15.png" xlink:type="simple"/></inline-formula> and its partial derivatives in which the highest order derivatives and nonlinear terms are involved. In the following,we give the main steps of this method:</p><p>Step 1. We use the wave transformation</p><disp-formula id="scirp.54539-formula42"><label>(2.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x16.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x17.png" xlink:type="simple"/></inline-formula> is a positive constant, to reduce Equation (2.1) to the following ODE:</p><disp-formula id="scirp.54539-formula43"><label>(2.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x18.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x19.png" xlink:type="simple"/></inline-formula> is a polynomial in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x20.png" xlink:type="simple"/></inline-formula> and its total derivatives,while <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x21.png" xlink:type="simple"/></inline-formula></p><p>Step 2. Suppose that the solution of ODE (2.3) can be expressed by a polynomial in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x22.png" xlink:type="simple"/></inline-formula> as follows</p><disp-formula id="scirp.54539-formula44"><label>(2.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x23.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x24.png" xlink:type="simple"/></inline-formula> satisfies the ODE in the form</p><disp-formula id="scirp.54539-formula45"><label>(2.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x25.png"  xlink:type="simple"/></disp-formula><p>the solutions of ODE (2.5) are when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x26.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x27.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula46"><label>(2.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x28.png"  xlink:type="simple"/></disp-formula><p>when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x29.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula47"><label>(2.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x30.png"  xlink:type="simple"/></disp-formula><p>when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x31.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula48"><label>(2.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x32.png"  xlink:type="simple"/></disp-formula><p>when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x33.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula49"><label>(2.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x34.png"  xlink:type="simple"/></disp-formula><p>when <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x35.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula50"><label>(2.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x36.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x37.png" xlink:type="simple"/></inline-formula> are constants to be determined later,</p><p>Step 3. Substitute Equation (2.4) along Equation (2.5) into Equation (2.3) and collecting all the terms of the same power<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x38.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x39.png" xlink:type="simple"/></inline-formula>and equating them to zero, we obtain a system of algebraic equa-</p><p>tions, which can be solved by Maple or Mathematica to get the values of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x40.png" xlink:type="simple"/></inline-formula>.</p><p>Step 4. substituting these values and the solutions of Equation (2.5) into Equation (2.3) we obtain the exact solutions of Equation (2.3).</p></sec><sec id="s3"><title>3. Application</title><sec id="s3_1"><title>3.1. Example 1: Dynamical System in a New Double-Chain Model of DNA</title><p>An attractive nonlinear model for the nonlinear science in the deoxyribonucleic acid (DNA). The dynamics of DNA molecules is one of the most fascinating problems of modern biophysics because it is at the basis of life. The DNA structure has been studied during last decades. The investigation of DNA dynamics has successfully predicted the appearance of important nonlinear structures. It has been shown that the nonlinearity is responsible for forming localized waves. These localized waves are interesting because they have the capability to transport energy without dissipation [<xref ref-type="bibr" rid="scirp.54539-ref30">30</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref38">38</xref>] . In Ref. [<xref ref-type="bibr" rid="scirp.54539-ref37">37</xref>] [<xref ref-type="bibr" rid="scirp.54539-ref38">38</xref>] , it is given that a new double-chain model of DNA consists of two long elastic homogeneous strands which represent two polynucleotide chains of the DNA mole- cule, connected with each other by an elastic membrane representing the hydrogen bonds between the base pair of the two chains. Under some appropriate approximation, the new double-chain model of DNA can be des- cribed by the following two general nonlinear dynamical system:</p><disp-formula id="scirp.54539-formula51"><label>(3.1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula52"><label>(3.2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x42.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.54539-formula53"><label>(3.3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x43.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x46.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x47.png" xlink:type="simple"/></inline-formula> denote respectively the mass density, the area of transverse cross-section, the Young’s modulus and tension density of each strand; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x48.png" xlink:type="simple"/></inline-formula>is the rigidity of the elastic membrance; <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x49.png" xlink:type="simple"/></inline-formula>is the distance between the two strands, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x50.png" xlink:type="simple"/></inline-formula> is the height of the membrance in the equilibrium positive. In Equations (3.1) and (3.2), <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x51.png" xlink:type="simple"/></inline-formula>is the difference of the longitudianl displacements of the bottom and top strands, while <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x52.png" xlink:type="simple"/></inline-formula> is the difference of the transverse displacements of the bottom and top strands.</p><p>we first introduce the transformation</p><disp-formula id="scirp.54539-formula54"><label>(3.4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x53.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x54.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x55.png" xlink:type="simple"/></inline-formula> are constants, to reduce Equations (3.1) and (3.2) to the following system of equations:</p><disp-formula id="scirp.54539-formula55"><label>(3.5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x56.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.54539-formula56"><label>(3.6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x57.png"  xlink:type="simple"/></disp-formula><p>Comparing Equations (3.5) and (3.6) and using (3.4) we deduce that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x58.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x59.png" xlink:type="simple"/></inline-formula>. Now Equations (3.5) and (3.6) can be written as</p><disp-formula id="scirp.54539-formula57"><label>(3.7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x60.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.54539-formula58"><label>(3.8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x61.png"  xlink:type="simple"/></disp-formula><p>The wave transformation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x62.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x63.png" xlink:type="simple"/></inline-formula>, reduce Equation (3.7) to the following ODE:</p><disp-formula id="scirp.54539-formula59"><label>(3.9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x64.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x65.png" xlink:type="simple"/></inline-formula>. Balancing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x66.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x67.png" xlink:type="simple"/></inline-formula> yields,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x68.png" xlink:type="simple"/></inline-formula>. Consequently, we have the formal solution:</p><disp-formula id="scirp.54539-formula60"><label>(3.10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x69.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x70.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x71.png" xlink:type="simple"/></inline-formula> are constants to be determined, such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x71.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x72.png" xlink:type="simple"/></inline-formula>. It is easy to see that</p><disp-formula id="scirp.54539-formula61"><label>(3.11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x73.png"  xlink:type="simple"/></disp-formula><p>substituting Equation (3.10) and its derivatives in Equation (3.9) and equating the coefficient of different power’s of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x74.png" xlink:type="simple"/></inline-formula> to zero, we get</p><disp-formula id="scirp.54539-formula62"><label>(3.12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula63"><label>(3.13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula64"><label>(3.14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula65"><label>(3.15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x78.png"  xlink:type="simple"/></disp-formula><p>Equations (3.12)-(3.15) yields</p><disp-formula id="scirp.54539-formula66"><graphic  xlink:href="http://html.scirp.org/file/4-2340163x79.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula67"><graphic  xlink:href="http://html.scirp.org/file/4-2340163x80.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula68"><graphic  xlink:href="http://html.scirp.org/file/4-2340163x81.png"  xlink:type="simple"/></disp-formula><p>Thus the solution is</p><disp-formula id="scirp.54539-formula69"><label>(3.16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x82.png"  xlink:type="simple"/></disp-formula><p>Let us now discuse the following case:</p><p>Case 1. if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x83.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula70"><label>(3.17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x84.png"  xlink:type="simple"/></disp-formula><p>Case 2. if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x85.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula71"><label>(3.18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x86.png"  xlink:type="simple"/></disp-formula><p>Case 3. if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x87.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula72"><label>(3.19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x88.png"  xlink:type="simple"/></disp-formula><p>Case 4. if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x89.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula73"><label>(3.20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x90.png"  xlink:type="simple"/></disp-formula><p>Case 5. if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x91.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula74"><label>(3.21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x92.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3_2"><title>3.2. Example 2. A Diffusive Predator-Prey System</title><p>Consider a system of two coupled nonlinear partial differential equations describing the spatio-temporal dyna- mics of a predator-prey system [<xref ref-type="bibr" rid="scirp.54539-ref39">39</xref>] ,</p><disp-formula id="scirp.54539-formula75"><label>(3.22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x93.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x94.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x95.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x96.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x97.png" xlink:type="simple"/></inline-formula> are positive parameters. The solutions of predator-prey system have been studied in various aspects [<xref ref-type="bibr" rid="scirp.54539-ref39">39</xref>] - [<xref ref-type="bibr" rid="scirp.54539-ref41">41</xref>] . The dynamics of the diffusive predator-prey system have assumed the following</p><p>relations between the parameters, namely <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x98.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x98.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x99.png" xlink:type="simple"/></inline-formula>. Under there assumptions, Equation (3.22) can be rewritten in the form:</p><disp-formula id="scirp.54539-formula76"><label>(3.23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x100.png"  xlink:type="simple"/></disp-formula><p>We use the wave transformation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x101.png" xlink:type="simple"/></inline-formula> to reduce Equation (3.23) to the following nonli- near system of ordinary differential equations:</p><disp-formula id="scirp.54539-formula77"><label>(3.24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x102.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x103.png" xlink:type="simple"/></inline-formula> is a nonzero constant.</p><p>In order to solve Equation (3.24), let us consider the following transformation</p><disp-formula id="scirp.54539-formula78"><label>(3.25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x104.png"  xlink:type="simple"/></disp-formula><p>Substituting the transformation (3.25) into Equation (3.24), we get</p><disp-formula id="scirp.54539-formula79"><label>(3.26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x105.png"  xlink:type="simple"/></disp-formula><p>Balancing <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x106.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x107.png" xlink:type="simple"/></inline-formula> in Equation (3.26) yields,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x108.png" xlink:type="simple"/></inline-formula>. Consequently, we get the same formal solution (3.10). Substituting Equation (3.10) and its derivatives in Equation (3.26) and equating the coefficient of different power's of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x109.png" xlink:type="simple"/></inline-formula> to zero, we get</p><disp-formula id="scirp.54539-formula80"><label>(3.27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x110.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula81"><label>(3.28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x111.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula82"><label>(3.29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x112.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula83"><label>(3.30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x113.png"  xlink:type="simple"/></disp-formula><p>Equations (3.27)-(3.30) yields</p><p>Case 1.</p><disp-formula id="scirp.54539-formula84"><graphic  xlink:href="http://html.scirp.org/file/4-2340163x114.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula85"><graphic  xlink:href="http://html.scirp.org/file/4-2340163x115.png"  xlink:type="simple"/></disp-formula><p>Case 2.</p><disp-formula id="scirp.54539-formula86"><graphic  xlink:href="http://html.scirp.org/file/4-2340163x116.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.54539-formula87"><graphic  xlink:href="http://html.scirp.org/file/4-2340163x117.png"  xlink:type="simple"/></disp-formula><p>Thus the solution is</p><p>Case 1.</p><disp-formula id="scirp.54539-formula88"><label>(3.31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x118.png"  xlink:type="simple"/></disp-formula><p>Case 2.</p><disp-formula id="scirp.54539-formula89"><label>(3.32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x119.png"  xlink:type="simple"/></disp-formula><p>Let us now discuss the following cases:</p><p>Case 1.</p><p>Case (1.1). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x120.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula90"><label>(3.33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x121.png"  xlink:type="simple"/></disp-formula><p>Case (1.2). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x122.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula91"><label>(3.34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x123.png"  xlink:type="simple"/></disp-formula><p>Case (1.3). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x124.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula92"><label>(3.35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x125.png"  xlink:type="simple"/></disp-formula><p>Case (1.4). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x126.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula93"><label>(3.36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x127.png"  xlink:type="simple"/></disp-formula><p>Case (1.5). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x128.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula94"><label>(3.37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x129.png"  xlink:type="simple"/></disp-formula><p>Case 2.</p><p>Case (2.1). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x130.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula95"><label>(3.38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x131.png"  xlink:type="simple"/></disp-formula><p>Case (2.2). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x132.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula96"><label>(3.39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x133.png"  xlink:type="simple"/></disp-formula><p>Case (2.3). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x134.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula97"><label>(3.40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x135.png"  xlink:type="simple"/></disp-formula><p>Case (2.4). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x136.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula98"><label>(3.41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x137.png"  xlink:type="simple"/></disp-formula><p>Case (2.5). if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x138.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.54539-formula99"><label>(3.42)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-2340163x139.png"  xlink:type="simple"/></disp-formula></sec></sec><sec id="s4"><title>4. Conclusion</title><p>We establish exact solutions for the dynamics of DNA molecules is one of the most fascinating problems of modern biophysics because it is at the basis of life. The DNA structure has been studied during last decades. The investigation of DNA dynamics has successfully predicted the appearance of important nonlinear structures and a system of two coupled nonlinear partial differential equations describing the spatio-temporal dynamics of a</p><p>predator-prey system where the prey per capita growth rate is subject to the Allee effect. The <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x140.png" xlink:type="simple"/></inline-formula>-</p><p>expansion method has been successfully used to find the exact traveling wave solutions of some nonlinear evolution equations. As an application, the traveling wave solutions for Dynamical system in a new Double- Chain Model of DNA and a diffuusive predator-prey system, which have been constructed using the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-2340163x141.png" xlink:type="simple"/></inline-formula>-</p><p>expansion method. Let us compare between our results obtained in the present article with the well-known results obtained by other authors using different methods as follows: Our results of Dynamical system in a new Double-Chain Model of DNA and a diffusive predator-prey system, are new and different from those obtained in [<xref ref-type="bibr" rid="scirp.54539-ref37">37</xref>] -[<xref ref-type="bibr" rid="scirp.54539-ref41">41</xref>] and <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> show the solitary traveling wave solution of Dynamical system in a new</p><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Solution of Equations (3.17)-(3.21). (a) Equations (3.17); (b) Equations (3.18); (c) Equations (3.19); (d) Equations (3.20); (e) Equations (3.21).</title></caption><fig id ="fig1_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x142.png"/></fig><fig id ="fig1_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x143.png"/></fig><fig id ="fig1_3"><label> (d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x144.png"/></fig><fig id ="fig1_4"><label>(e)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x145.png"/></fig><fig id ="fig1_5"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x146.png"/></fig></fig-group><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> Solution of Equations (3.38)-(3.42). (a) Equations (3.38); (b) Equations (3.39); (c) Equations (3.40); (d) Equations (3.41); (e) Equations (3.42).</title></caption><fig id ="fig2_1"><label> (b)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x147.png"/></fig><fig id ="fig2_2"><label>(c)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x148.png"/></fig><fig id ="fig2_3"><label> (d)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x149.png"/></fig><fig id ="fig2_4"><label>(e)</label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x150.png"/></fig><fig id ="fig2_5"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/4-2340163x151.png"/></fig></fig-group><p>Double-Chain Model of DNA and a diffusive predator-prey system. It can be concluded that this method is reliable and proposes a variety of exact solutions NPDEs. The performance of this method is effective and can be applied to many other nonlinear evolution equations.</p></sec><sec id="s5"><title>Cite this paper</title><p>Mahmoud A. E.Abdelrahman,Emad H. M.Zahran,Mostafa M. A.Khater, (2015) The exp(-&amp;phi;(&amp;xi;))-Expansion Method and Its Application for Solving Nonlinear Evolution Equations. International Journal of Modern Nonlinear Theory and Application,04,37-47. doi: 10.4236/ijmnta.2015.41004</p></sec><sec id="s6"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.54539-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ablowitz, M.J. and Segur, H. (1981) Solitions and Inverse Scattering Transform. 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