<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">AM</journal-id><journal-title-group><journal-title>Applied Mathematics</journal-title></journal-title-group><issn pub-type="epub">2152-7385</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/am.2015.61016</article-id><article-id pub-id-type="publisher-id">AM-53339</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>
 
 
  Travelling Wave Solutions of Kaup-Kupershmidt Equation Which Describes Pseudo Spherical Surfaces
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>.</surname><given-names>M. Gharib</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>Mathematics Department, College of Science and Information Technology, Zarqa University, Zarqa, Jordan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>Gharibmusa@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>01</month><year>2015</year></pub-date><volume>06</volume><issue>01</issue><fpage>163</fpage><lpage>172</lpage><history><date date-type="received"><day>1</day>	<month>December</month>	<year>2014</year></date><date date-type="rev-recd"><day>accepted</day>	<month>16</month>	<year>December</year>	</date><date date-type="accepted"><day>19</day>	<month>January</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>
 
 
  In this paper I introduce the geometric notion of a differential system describing surfaces of a constant negative curvature and describe a family of pseudo-spherical surface for Kaup-Ku-pershmidt Equation with constant Gaussian curvature 
  –1. I obtained new soliton solutions for Kaup-Kupershmidt Equation by using the modified sine-cosine method.
 
</p></abstract><kwd-group><kwd>Soliton Solutions</kwd><kwd> Pseudo Spherical Surfaces</kwd><kwd> Nonlinear Evolution Equations</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Many partial differential equations which continue to be investigated due to their role in mathematics and physics exhibit interrelationships with the geometry of surfaces, or submanifolds, immersed in a three-dimensional space [<xref ref-type="bibr" rid="scirp.53339-ref1">1</xref>] . In particular, it has been known for a while that there is a relationship between surfaces of a constant negative Gaussian curvature in Euclidean three-space, the Sine-Gordon Equation and B&#228;cklund transformations which are relevant to the given equation [<xref ref-type="bibr" rid="scirp.53339-ref2">2</xref>] . Moreover, the original B&#228;cklund transformation for the Sine-Gor- don Equation is also a simple geometric construction for pseudospherical surfaces [<xref ref-type="bibr" rid="scirp.53339-ref3">3</xref>] -[<xref ref-type="bibr" rid="scirp.53339-ref5">5</xref>] . It is well known that nonlinear complex physical phenomena are related to nonlinear partial diﬀerential equations (NLPDEs) which are involved in many fields from physics to biology, chemistry, mechanics, etc.</p><p>As mathematical models of the phenomena, the investigation of exact solutions to the NLPDEs reveals to be very important for the understanding of these physical problems. Many mathematicians and physicists have well understood this importance when they decided to pay special attention to the development of sophisticated methods for constructing exact solutions to the NLPDEs. Thus, a number of powerful methods have been presented.</p><p>We can cite the inverse scattering transform [<xref ref-type="bibr" rid="scirp.53339-ref6">6</xref>] , the B&#228;cklund and Darboux transform [<xref ref-type="bibr" rid="scirp.53339-ref7">7</xref>] - [<xref ref-type="bibr" rid="scirp.53339-ref10">10</xref>] , Hirota’s bilinear method [<xref ref-type="bibr" rid="scirp.53339-ref11">11</xref>] , the homogeneous balance method [<xref ref-type="bibr" rid="scirp.53339-ref12">12</xref>] , Jacobi elliptic function method [<xref ref-type="bibr" rid="scirp.53339-ref13">13</xref>] , the tanh method and extended tanh-function method [<xref ref-type="bibr" rid="scirp.53339-ref14">14</xref>] - [<xref ref-type="bibr" rid="scirp.53339-ref20">20</xref>] , F-expansion method [<xref ref-type="bibr" rid="scirp.53339-ref21">21</xref>] - [<xref ref-type="bibr" rid="scirp.53339-ref23">23</xref>] and so on. The notion of conservation laws is important in the study of nonlinear evolution equations (NLEEs) appearing in mathematical physics [<xref ref-type="bibr" rid="scirp.53339-ref24">24</xref>] .</p><p>Consider Kaup-Kupershmidt Equation,</p><disp-formula id="scirp.53339-formula240"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x5.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x6.png" xlink:type="simple"/></inline-formula> is a function of two independent variables <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x7.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x8.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s2"><title>2. Kaup-Kupershmidt Equation Which Describes Pseudo Spherical Surfaces</title><p>I recall the definition [<xref ref-type="bibr" rid="scirp.53339-ref25">25</xref>] -[<xref ref-type="bibr" rid="scirp.53339-ref28">28</xref>] of a differential equation (DE) that describes a pss. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x9.png" xlink:type="simple"/></inline-formula> be a two dimensional differentiable manifold with coordinates<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x10.png" xlink:type="simple"/></inline-formula>. A DE for a real function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x11.png" xlink:type="simple"/></inline-formula> describes a pss if it is a necessary and sufficient condition for the existence of differentiable functions</p><disp-formula id="scirp.53339-formula241"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x12.png"  xlink:type="simple"/></disp-formula><p>depending on u and its derivatives such that the one-forms</p><disp-formula id="scirp.53339-formula242"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x13.png"  xlink:type="simple"/></disp-formula><p>satisfy the structure equations of a pss, i.e.,</p><disp-formula id="scirp.53339-formula243"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x14.png"  xlink:type="simple"/></disp-formula><p>I obtain that the Kaup-Kupershmidt Equation (1) describes pseudospherical surfaces, with associated one forms <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x15.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x16.png" xlink:type="simple"/></inline-formula> given by</p><disp-formula id="scirp.53339-formula244"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x17.png"  xlink:type="simple"/></disp-formula><p>As a consequence, each solution of the DE provides a local metric on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x18.png" xlink:type="simple"/></inline-formula>, whose Gaussian curvature is constant, equal to −1. Moreover, the above definition is equivalent to saying that DE for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x19.png" xlink:type="simple"/></inline-formula> is the integrability condition for the problem [<xref ref-type="bibr" rid="scirp.53339-ref19">19</xref>] [<xref ref-type="bibr" rid="scirp.53339-ref29">29</xref>] :</p><disp-formula id="scirp.53339-formula245"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x20.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x21.png" xlink:type="simple"/></inline-formula> denotes exterior differentiation, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x22.png" xlink:type="simple"/></inline-formula>is a column vector and the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x23.png" xlink:type="simple"/></inline-formula> matrix <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x24.png" xlink:type="simple"/></inline-formula> is traceless</p><disp-formula id="scirp.53339-formula246"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x25.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Exact Solution for Kaup-Kupershmidt Equation</title><p>With the rapid development of science and technology, the study kernel of modern science is changed from linear to nonlinear step by step. Many nonlinear science problems can simply and exactly be described by using the mathematical model of nonlinear equation. Up to now, many important physical nonlinear evolution equations are found, such as Sine-Gordon Equation, KdV Equations, Schrodinger Equation all possess solitary wave solutions. There exist many methods to seek for the solitary wave solutions, such as inverse scattering method, Hopf-Cole transformation, Miura transformations, Darboux transformation and B&#228;cklund transformation [<xref ref-type="bibr" rid="scirp.53339-ref7">7</xref>] -[<xref ref-type="bibr" rid="scirp.53339-ref10">10</xref>] , but solving nonlinear equations is still an important task [<xref ref-type="bibr" rid="scirp.53339-ref27">27</xref>] -[<xref ref-type="bibr" rid="scirp.53339-ref30">30</xref>] . In this paper, with the aid of Mathematica, a traveling wave solution for a class of Kaup-Kupershmidt Equation,</p><disp-formula id="scirp.53339-formula247"><graphic  xlink:href="http://html.scirp.org/file/16-7402219x26.png"  xlink:type="simple"/></disp-formula><p>In order to obtain the soliton solution of (1), I will use the modified sine-cosine to develop traveling wave solutions to this equation. The modified sine-cosine method admits the use of solutions [<xref ref-type="bibr" rid="scirp.53339-ref30">30</xref>]</p><disp-formula id="scirp.53339-formula248"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x27.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.53339-formula249"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x28.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x29.png" xlink:type="simple"/></inline-formula> is the soliton amplitude, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x30.png" xlink:type="simple"/></inline-formula>is the width of the soliton, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x31.png" xlink:type="simple"/></inline-formula>is the soliton velocity and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x32.png" xlink:type="simple"/></inline-formula> is constant to be determined later, the unknown index <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x29.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x33.png" xlink:type="simple"/></inline-formula> will be determined during the course of derivation of the solution of Equation (8). From Equation (8), I obtain</p><disp-formula id="scirp.53339-formula250"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x34.png"  xlink:type="simple"/></disp-formula><p>From Equation (9), I obtain</p><disp-formula id="scirp.53339-formula251"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x35.png"  xlink:type="simple"/></disp-formula><p>With the aid of Mathematica or Maple, from (8) and (10), we can get</p><disp-formula id="scirp.53339-formula252"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x36.png"  xlink:type="simple"/></disp-formula><p>Now, from Equation (12) equating the exponents n − 5 and 2n − 3 leads<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x37.png" xlink:type="simple"/></inline-formula>, which gives<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x38.png" xlink:type="simple"/></inline-formula>, such that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x39.png" xlink:type="simple"/></inline-formula></p><p>Also from Equation (12) equating the coefficients of like powers of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x40.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x41.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x42.png" xlink:type="simple"/></inline-formula> to zero, I get</p><disp-formula id="scirp.53339-formula253"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x43.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53339-formula254"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x44.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.53339-formula255"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x45.png"  xlink:type="simple"/></disp-formula><p>Solving the above system by the aid of Wu elimination method [<xref ref-type="bibr" rid="scirp.53339-ref31">31</xref>] , I obtain the three solutions</p><disp-formula id="scirp.53339-formula256"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x46.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.53339-formula257"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x47.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.53339-formula258"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/16-7402219x48.png"  xlink:type="simple"/></disp-formula><p>Then the soliton solutions of the Kaup-Kupershmidt Equation is given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x49.png" xlink:type="simple"/></inline-formula>see <xref ref-type="fig" rid="fig1">Figure 1</xref> and <xref ref-type="fig" rid="fig2">Figure 2</xref> (19)</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x50.png" xlink:type="simple"/></inline-formula>see <xref ref-type="fig" rid="fig3">Figure 3</xref> and <xref ref-type="fig" rid="fig4">Figure 4</xref> (20)</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x51.png" xlink:type="simple"/></inline-formula>see <xref ref-type="fig" rid="fig5">Figure 5</xref> and <xref ref-type="fig" rid="fig6">Figure 6</xref> (21)</p><p>If setting<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x52.png" xlink:type="simple"/></inline-formula>, then the solutions (19) and (21) are given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x53.png" xlink:type="simple"/></inline-formula>see <xref ref-type="fig" rid="fig7">Figure 7</xref> and <xref ref-type="fig" rid="fig8">Figure 8</xref> (22)</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x54.png" xlink:type="simple"/></inline-formula>see <xref ref-type="fig" rid="fig9">Figure 9</xref> and <xref ref-type="fig" rid="fig1">Figure 1</xref>0 (23)</p><p>and</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x55.png" xlink:type="simple"/></inline-formula>see <xref ref-type="fig" rid="fig1">Figure 1</xref>1 and <xref ref-type="fig" rid="fig1">Figure 1</xref>2 (24)</p><p>The double-kink solutions (19), (20), and (21) are characterized by the eigenvalue <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x56.png" xlink:type="simple"/></inline-formula> (see Figures 1-6). The solutions (22), (23) and (24) are the single-soliton solutions (see Figures 7-12) corresponding to the eigenvalue<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x57.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Conclusions</title><p>The new types of exact traveling wave solution obtained in this paper for the Kaup-Kupershmidt Equation will</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref6">6</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x59.png" xlink:type="simple"/></inline-formula> is shown at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x60.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x61.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x59.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x60.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x62.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x58.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref20">20</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x64.png" xlink:type="simple"/></inline-formula> is shown at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x65.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x65.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x66.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x63.png"/></fig><fig id="fig3"  position="float"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref6">6</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x68.png" xlink:type="simple"/></inline-formula> is shown at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x69.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x70.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x68.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x71.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x67.png"/></fig><fig id="fig4"  position="float"><label><xref ref-type="fig" rid="fig4">Figure 4</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref20">20</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x73.png" xlink:type="simple"/></inline-formula> is shown at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x74.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x74.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x75.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x72.png"/></fig><fig id="fig5"  position="float"><label><xref ref-type="fig" rid="fig5">Figure 5</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref6">6</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x77.png" xlink:type="simple"/></inline-formula> is shown at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x78.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x79.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x78.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x79.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x80.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x76.png"/></fig><fig id="fig6"  position="float"><label><xref ref-type="fig" rid="fig6">Figure 6</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref20">20</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x82.png" xlink:type="simple"/></inline-formula> is shown at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x83.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x83.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x84.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x81.png"/></fig><fig id="fig7"  position="float"><label><xref ref-type="fig" rid="fig7">Figure 7</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref6">6</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x86.png" xlink:type="simple"/></inline-formula> is shown at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x87.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x88.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x86.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x87.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x89.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x85.png"/></fig><fig id="fig8"  position="float"><label><xref ref-type="fig" rid="fig8">Figure 8</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref20">20</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x91.png" xlink:type="simple"/></inline-formula> is shown at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x92.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x93.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x90.png"/></fig><fig id="fig9"  position="float"><label><xref ref-type="fig" rid="fig9">Figure 9</xref></label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref6">6</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x95.png" xlink:type="simple"/></inline-formula> is shown at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x96.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x97.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x98.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x94.png"/></fig><fig id="fig10"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>0</label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref20">20</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x100.png" xlink:type="simple"/></inline-formula> is shown at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x101.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x100.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x102.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x99.png"/></fig><fig id="fig11"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>1</label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref6">6</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x104.png" xlink:type="simple"/></inline-formula> is shown at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x105.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x106.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x104.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x105.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x106.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x107.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x103.png"/></fig><fig id="fig12"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref>2</label><caption><title> See [<xref ref-type="bibr" rid="scirp.53339-ref20">20</xref>] : solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x109.png" xlink:type="simple"/></inline-formula> is shown at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x110.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/16-7402219x111.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/16-7402219x108.png"/></fig><p>be of benefit to future studies.</p><p>The Soliton Equations play a central role in the field of integrable systems and also play a fundamental role in several other areas of mathematics and physics.</p><p>A soliton is a localized pulse-like nonlinear wave that possesses remarkable stability properties. Typically, problems that admit soliton solutions are in the form of evolution equations that describe how some variable or a set of variables evolves in time from a given state. The equations may take a variety of forms, for example, PDEs, differential difference equations, partial difference equations, integro-differential equations, as well as coupled ODEs of finite order.</p><p>In this paper, we considered the construction of exact solutions to Kaup-Kupershmidt Equation. I obtain travelling wave solutions for the above equation by using the modified sine-cosine method with the aid of Mathematica.</p><p>A travelling wave of permanent form has already been met; this is the solitary wave solution of the nonlinear evolution equation itself. Such a wave is a special solution of the governing equation which does not change its shape and propagates at constant speed.</p><p>The soliton phenomena of nonlinear evolution equations represent an important and well-established field of modern physics, mathematical physics and applied mathematics. Solitons are found in various areas of physics from hydrodynamics and plasma physics, nonlinear optics and solid state physics, to field theory and gravitation. NLEEs which describe soliton phenomena have a universal character.</p></sec><sec id="s5"><title>Funding</title><p>This research is funded by the Deanship of Research and Graduate Studies in Zarqa University/Jordan.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.53339-ref1"><label>1</label><mixed-citation publication-type="book" xlink:type="simple">Rogers, C. and Schief, W.F. (2002) B&amp;auml;cklund and Darboux Transformations, Geometry and Modern Applications in Soliton Theory. 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