<?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.2014.513186</article-id><article-id pub-id-type="publisher-id">AM-47692</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>COMPUTER SCIENCE &amp; COMMUNICATIONS</subject><subject>ENGINEERING</subject><subject>PHYSICS &amp; MATHEMATICS</subject></subj-group></article-categories><title-group><article-title>A New Approach for the Exact Solutions of Nonlinear Equations of Fractional Order via Modified Simple Equation Method</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Muhammad</surname><given-names>Younis</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>Centre for Undergraduate Studies, University of the Punjab, Lahore, Pakistan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>younis.pu@gmail.com</email></corresp></author-notes><pub-date pub-type="epub"><day>07</day><month>07</month><year>2014</year></pub-date><volume>05</volume><issue>13</issue><fpage>1927</fpage><lpage>1932</lpage><history><date date-type="received"><day>12</day>	<month>April</month>	<year>2014</year></date><date date-type="rev-recd"><day>23</day>	<month>May</month>	<year>2014</year>	</date><date date-type="accepted"><day>1</day>	<month>June</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
	In this article,
the modified simple equation method has been extended to celebrate the exact solutions
of nonlinear partial time-space differential equations of fractional order.
Firstly, the fractional complex transformation has been implemented to convert
nonlinear partial fractional differential equations into nonlinear ordinary
differential equations. Afterwards, modified simple equation method has been
implemented, to find the exact solutions of these equations, in the sense of
modified Riemann-Liouville derivative. For applications, the exact solutions of
time-space fractional derivative Burgers’ equation and time-space fractional
derivative foam drainage equation have been discussed. Moreover, it can also be
concluded that the proposed method is easy, direct and concise as compared to
other existing methods.
</p></abstract><kwd-group><kwd>Exact Solutions</kwd><kwd> Complex Transformation</kwd><kwd> Modified Simple Equation Method</kwd><kwd> Nonlinear Equations of Fractional Order</kwd><kwd> Fractional Calculus Theory</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Nonlinear partial differential equations have shown a variety of applications in almost every field of life, such as in electromagnetics, acoustics, electrochemistry, cosmology, biological and material science [<xref ref-type="bibr" rid="scirp.47692-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.47692-ref4">4</xref>] . Fractional differential equations can be considered as the general form of the differential equations, as they are involved with the derivatives of any real or complex order (for details see [<xref ref-type="bibr" rid="scirp.47692-ref3">3</xref>] ).</p><p>Knowing the importance of differential equations of fractional order, lots of authors are working to find the exact or numerical solutions of the equations. For examples, the adomian decomposition method [<xref ref-type="bibr" rid="scirp.47692-ref5">5</xref>] , Pade approximation method [<xref ref-type="bibr" rid="scirp.47692-ref6">6</xref>] and generalized differential transform method [<xref ref-type="bibr" rid="scirp.47692-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.47692-ref8">8</xref>] have been used to find the numerical solutions for fractional order differential equations. The <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\4a8482bf-1c22-4eaa-a9e6-503dbf1d2cd4.png" xlink:type="simple"/></inline-formula>-expansion method was introduced, by Wang et al. [<xref ref-type="bibr" rid="scirp.47692-ref9">9</xref>] , to find the travelling wave solutions of nonlinear evolution equations. This method was further extended [<xref ref-type="bibr" rid="scirp.47692-ref10">10</xref>] [<xref ref-type="bibr" rid="scirp.47692-ref11">11</xref>] to find the solutions of fractional order differential equations, the Jacobi elliptic function expansion method [<xref ref-type="bibr" rid="scirp.47692-ref12">12</xref>] , the tanh-function method for finding solitary wave solutions [<xref ref-type="bibr" rid="scirp.47692-ref13">13</xref>] , the homotopy perturbation method [<xref ref-type="bibr" rid="scirp.47692-ref14">14</xref>] , the first integral method [<xref ref-type="bibr" rid="scirp.47692-ref15">15</xref>] , the solitary wave ansatz [<xref ref-type="bibr" rid="scirp.47692-ref16">16</xref>] etc.</p><p>In this article, a new approach has been developed to find the exact solutions of nonlinear partial differential equations of fractional order by the fractional complex transformation [<xref ref-type="bibr" rid="scirp.47692-ref17">17</xref>] and modified simple equation method [<xref ref-type="bibr" rid="scirp.47692-ref18">18</xref>] [<xref ref-type="bibr" rid="scirp.47692-ref19">19</xref>] , in the sense of modified Riemann-Liouville derivative. For this, we first use the fractional complex transformation on these equations to convert into ordinary differential equations. Then, the modified simple equation method can be applied to find the exact solutions. Two applications are being considered to find the solution of nonlinear Burgers’ equation with time-space fractional derivatives, which has the following form [<xref ref-type="bibr" rid="scirp.47692-ref5">5</xref>] :</p><disp-formula id="scirp.47692-formula534"><label>(1.1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\b9cc00e2-1883-428d-b62e-469585773f17.png"/></disp-formula><p>and time-spce fractioanl derivative foam drainage equation [<xref ref-type="bibr" rid="scirp.47692-ref11">11</xref>] :</p><disp-formula id="scirp.47692-formula535"><label>(1.2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\190be3bd-55dd-439a-bb2a-1392c86d1d48.png"/></disp-formula><p>The rest of the article is organized as follows, in section 2 the basic definitions and properties of the fractional theory are considered regrading to modified Riemann-Liouville derivative. In section 3, the modified simple equation method has been proposed to find the exact solutions for NPDEs of fractional order with the help of fractional complex transformation. The two applications are being considered to find the exact solution in section 4. In last section 5, the conclusion has been drawn.</p></sec><sec id="s2"><title>2. Preliminaries and Basic Definitions</title><p>In this section, the extended method has been applied in the sense of the Jumarie’s modified Riemann-Liouville derivative of order<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\a4eb2a31-b15d-4ec6-b7ab-2dfbab51a731.png" xlink:type="simple"/></inline-formula>. For this, some basic definitions and properties of the fractional calculus theory are being considered (for details see [<xref ref-type="bibr" rid="scirp.47692-ref3">3</xref>] ). Thus, the fractional integral and derivatives can be defined following [<xref ref-type="bibr" rid="scirp.47692-ref20">20</xref>] [<xref ref-type="bibr" rid="scirp.47692-ref21">21</xref>] :</p><p>Definition 2.1 A real function<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\c54d2c1f-3da0-4e82-8d81-08e3d7e8b0f4.png" xlink:type="simple"/></inline-formula>, is said to be in the space<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\408715d7-8c75-4a36-aa61-06905145d3d7.png" xlink:type="simple"/></inline-formula>, if there exists a real number <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\6642b767-2308-4710-894d-4289449895e2.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\22ad35d6-34f8-47c8-bede-09ca6ddbb5bd.png" xlink:type="simple"/></inline-formula>, where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\f5445b59-b108-4e48-a8c9-c2deed2dfa59.png" xlink:type="simple"/></inline-formula>, and it is said to be in the space <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\1dd198f4-6684-43d6-bc3d-f8b133224883.png" xlink:type="simple"/></inline-formula> if<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\25f98f8d-0966-49d7-9dbd-224e35cbbb4c.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\7eba199f-1aea-4731-8835-046ba94f1687.png" xlink:type="simple"/></inline-formula>.</p><p>Definition 2.2 The Jumarie’s modified Riemann-Liouville derivative, of order<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\d1c4120a-3211-442f-bfa9-a183bb09ba84.png" xlink:type="simple"/></inline-formula>, can be defined by the following expression:</p><disp-formula id="scirp.47692-formula536"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\471a3043-d13a-424e-b987-14ca2887938c.png"/></disp-formula><p>Moreover, some properties for the modified Riemann-Liouville derivative have also been given as follows:</p><disp-formula id="scirp.47692-formula537"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\55a5467f-c406-4e25-9cf0-b857d00f0adf.png"/></disp-formula><disp-formula id="scirp.47692-formula538"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\55a5467f-c406-4e25-9cf0-b857d00f0adf.png"/></disp-formula><disp-formula id="scirp.47692-formula539"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\55a5467f-c406-4e25-9cf0-b857d00f0adf.png"/></disp-formula></sec><sec id="s3"><title>3. The Modified Simple Equation Method</title><p>In this section, the modified simple equation method [<xref ref-type="bibr" rid="scirp.47692-ref18">18</xref>] has been discussed to obtain the solutions of nonlinear partial differential equations of fractional order, in very easy way.</p><p>For this, we consider the following NPDE of fractional order:</p><disp-formula id="scirp.47692-formula540"><label>(3.1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\b97e3238-0217-452a-a007-0d01f06f19c8.png"/></disp-formula><p>where u is an unknown function and P is a polynomial of u and its partial fractional derivatives along with the involvement of higher order derivatives and nonlinear terms.</p><p>To find the exact solutions, the method can be performed using the following steps.</p><p>Step 1: First, we convert the NPDE of fractional order into nonlinear ordinary differential equations using fractional complex transformation introduced by Li et al. [<xref ref-type="bibr" rid="scirp.47692-ref17">17</xref>] .</p><p>The travelling wave variable</p><disp-formula id="scirp.47692-formula541"><label>(3.2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\b0e892b1-a660-4b0f-bcd7-15a0fa6bf4cb.png"/></disp-formula><p>where K, L and M are non-zero arbitrary constants, permits us to reduce Equation (3.2) to an ODE of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\8d735816-a4cf-4dc2-b848-95b521b7f550.png" xlink:type="simple"/></inline-formula> in the following form</p><disp-formula id="scirp.47692-formula542"><label>(3.3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\9feb6fcc-723e-4928-bc81-5568476c80ef.png"/></disp-formula><p>Step 2: Suppose that the solution of Equation (3.3) can be expressed as a polynomial of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\0cba2fd6-a677-468c-b08a-644d46ad1397.png" xlink:type="simple"/></inline-formula> in the form:</p><disp-formula id="scirp.47692-formula543"><label>(3.4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\fd64fee7-7c07-40da-9199-b86fe732a9fe.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\9161628e-d65b-482d-957a-448f8e58acc8.png" xlink:type="simple"/></inline-formula>s are arbitrary constants.</p><p>Step 3: The homogeneous balance can be used, to determine the positive integer m, between the highest order derivatives and the nonlinear terms appearing in (3.4).</p><p>Step 4: After the substitution of (3.4) into (3.3), we collect all the terms with the same order of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\81b6eaed-dd93-4834-b939-e04fd3fccd96.png" xlink:type="simple"/></inline-formula> together. Equate each coefficient of the obtained polynomial to zero, yields the set of algebraic equations for <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\eb0467cd-1112-4304-8264-2ae88086ee41.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\274a2478-19bd-454c-96ea-fe042c65e2ec.png" xlink:type="simple"/></inline-formula>.</p><p>Step 5: After solving the system of algebraic equations, the variety of exact solutions can be celebrated.</p></sec><sec id="s4"><title>4. Applications to the Modified Simple Equation Method</title><p>In the following subsections, two applications (given in Equations (1.1) and (1.2)) are being considered to find the exact solutions by the proposed method.</p><sec id="s4_1"><title>4.1. Nonlinear Time-Space Fractional Burgers’ Equation</title><p>In this section, the modified simple equation method has been applied to construct the exact solutions for the nonlinear space-time fractional Burgers’ Equation (1.1). It can be observed that the fractional complex transform</p><disp-formula id="scirp.47692-formula544"><label>(4.1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\ed0a8ade-0883-4ccb-9420-5ebf7df20a66.png"/></disp-formula><p>where K and L are constants, permits to reduce the Equation (1.1) into an ODE of the following form:</p><disp-formula id="scirp.47692-formula545"><label>(4.2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\5f2a8f26-4afc-4f7f-8ad6-16d245752658.png"/></disp-formula><p>Now by calculating the homogeneous balance (i.e.,<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\5a8b3d68-4c6c-4622-a505-643b1d2c4da8.png" xlink:type="simple"/></inline-formula>), between the highest order derivatives and nonlinear term presented in the above equation, we have the following form</p><disp-formula id="scirp.47692-formula546"><label>(4.3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\de375db6-867c-4b6e-bbaf-01e59520f1b5.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\dd055228-4cfc-4971-9eef-1d69f57bd582.png" xlink:type="simple"/></inline-formula> and L are arbitrary constants. To determine these constants substitute the Equation (4.3) into (4.2), and collecting all the terms with the same power of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\1483baaa-3875-41cf-ab66-30b1fe533569.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\e2d784d1-f4ed-446a-9237-95c9432c7cf1.png" xlink:type="simple"/></inline-formula> together, equating each coefficient equal to zero, yields a set of algebraic equations.</p><disp-formula id="scirp.47692-formula547"><label>(4.4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\bd6ab261-0e2a-4da7-83e4-ced71b5cbe2c.png"/></disp-formula><disp-formula id="scirp.47692-formula548"><label>(4.5)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\de213d51-c675-40ef-8df1-069bcbc64a75.png"/></disp-formula><p>and</p><disp-formula id="scirp.47692-formula549"><label>(4.6)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\83801ebf-b5e7-46e2-b62e-0e73f7a54155.png"/></disp-formula><p>The above Equation (4.6), yields the value<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\b88dd0e3-e4a9-4833-b29f-285c04373ede.png" xlink:type="simple"/></inline-formula>.</p><p>The general solution of the Equation (4.4) is</p><disp-formula id="scirp.47692-formula550"><label>(4.7)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\21b905ca-9022-4e2b-aea8-a677be1c562a.png"/></disp-formula><p>While <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\c73117a0-c66b-4a05-ad01-e8495d0dde7e.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\ddfb6c97-16c3-4914-bd25-4e5b77f11706.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Consequently to this, the exact solution of the Equation (1.1) has the following form</p><disp-formula id="scirp.47692-formula551"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\669c8cbf-76d8-4fbb-a2f6-4f82895b75ae.png"/></disp-formula><p>For, the value <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\a94d231e-50b9-4f33-86ba-a3e3f633e2ef.png" xlink:type="simple"/></inline-formula> the Equation (4.5) reduces to</p><disp-formula id="scirp.47692-formula552"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\050d1d9e-3da5-41a5-b070-6e3003357d35.png"/></disp-formula><p>which also gives the same results.</p></sec><sec id="s4_2"><title>4.2. Nonlinear Time-Space Fractional Derivative Foam Drainage Equation</title><p>Applying the fractional complex transformation on the Equation (1.2), which reduces into the following form:</p><disp-formula id="scirp.47692-formula553"><label>(4.8)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\29179902-8039-427b-8cef-60155c82dccc.png"/></disp-formula><p>Now by calculating the homogeneous balance, which is<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\15c45fa6-6eb2-4e19-a3be-667035d5311d.png" xlink:type="simple"/></inline-formula>. We have the following form of the Equation (3.4)</p><disp-formula id="scirp.47692-formula554"><label>(4.9)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\0dadf28c-a998-49b1-ba40-f895e27100fc.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\f222a3f8-96d9-4c45-b02d-cd205d7fbd66.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\8e01ac9b-29e5-4da4-858b-403a443df937.png" xlink:type="simple"/></inline-formula> are arbitrary constants. To determine these constants, equate the coefficients of<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\42076e14-2180-43e0-a9d5-ba5c10be0ba4.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\d31d7615-49b8-4e53-a22f-42dd601ea274.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\c493bf1a-c210-47b0-9dd4-6ac76d6a2429.png" xlink:type="simple"/></inline-formula> equal to zero, yields the set of algebraic equations.</p><disp-formula id="scirp.47692-formula555"><label>(4.10)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\ef8b1b8d-7549-4dac-b1ba-4f35660d44fd.png"/></disp-formula><disp-formula id="scirp.47692-formula556"><label>(4.11)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\e6087921-98b6-4d47-86d6-9358c9f5693a.png"/></disp-formula><disp-formula id="scirp.47692-formula557"><label>(4.12)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\b23f0085-39c2-41d0-b6f0-7ae2f3506a79.png"/></disp-formula><p>and</p><disp-formula id="scirp.47692-formula558"><label>(4.13)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\d23c9bde-6ab5-4b4a-a314-c8456ed6636f.png"/></disp-formula><p>The above Equation (4.13), yields the value<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\bcb5e038-2fc7-42b5-87d7-ed7e4cfa2ef5.png" xlink:type="simple"/></inline-formula>.</p><p>Case 1: The general solution of the Equation (4.10) is</p><disp-formula id="scirp.47692-formula559"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\5d90a448-e7ed-4ce1-a346-a59dce66c9ba.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\23e1d4a1-91d7-4a79-9bcc-167a181b47bd.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\bb0c1166-2805-49a4-a872-4ff96e01e861.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Consequently to this, the exact solution of the Equation (1.2) has the following form</p><disp-formula id="scirp.47692-formula560"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\0126c578-9888-4c77-99a2-ab48d009025e.png"/></disp-formula><p>Case 2: For the value<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\7ba5e5f8-cfb0-4bdb-9506-037590ba26f3.png" xlink:type="simple"/></inline-formula>, the general solution of the equation (4.11) is</p><disp-formula id="scirp.47692-formula561"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\2a5e3e5c-ff55-4453-a579-ce28df91c6d6.png"/></disp-formula><p>while <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\675ebe16-d62b-4195-8a2f-2a7a8244b9be.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\c05d9294-3b66-4853-9c73-507a0925734e.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Consequently to this, the exact solution of the Equation (4.1) has the following form</p><disp-formula id="scirp.47692-formula562"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\adaf8063-23db-424d-a89a-047c1a0b0a70.png"/></disp-formula><p>Case 3: For the value<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\eed4cf22-1def-46cd-a2e7-41dfa3400516.png" xlink:type="simple"/></inline-formula>, the general solution of the Equation (4.12) is</p><disp-formula id="scirp.47692-formula563"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\2df7e825-9aec-4bab-a194-6ac49d78a3f2.png"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\ed0c80ba-41ad-4d78-9387-ce1af3b9295b.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\9844a6b9-82f6-45f7-9a28-ccb8a3f325ab.png" xlink:type="simple"/></inline-formula> are arbitrary constants. Consequently to this, the exact solution of the Equation (1.2) has the following form</p><disp-formula id="scirp.47692-formula564"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\9-7402160x\dfb7f895-7f41-4185-a415-67a59b0fbab5.png"/></disp-formula><p>Which are the required results.</p></sec></sec><sec id="s5"><title>5. Conclusion</title><p>The modified simple equation method has been extended to solve the nonlinear partial differential equation of fractional order, in the sense of modified Riemann-Liouville derivative. First, the fractional complex transformation has been used to convert the fractional order differential equations into ordinary differential equations. Then, the modified simple equation method has been used to find the exact solutions. The two applications have been considered to find the new exact solutions for the nonlinear time-space fractional derivative Burgers’ equation and time-space fractional derivative foam drainage equation. It can also be concluded that the proposed method is very simple, reliable and a variety of exact solutions to NPDEs of fractional order are proposed.</p></sec></body><back><ref-list><title>References</title><ref id="scirp.47692-ref1"><label>1</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>JOHNSON</surname><given-names> R.S. </given-names></name>,<etal>et al</etal>. (<year>1970</year>)<article-title>A NON-LINEAR EQUATION INCORPORATING DAMPING AND DISPERSION</article-title><source>. JOURNAL OF FLUID MECHANICS</source><volume> 42</volume>,<fpage> 49</fpage>-<lpage>60</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1017/S0022112070001064</pub-id></mixed-citation></ref><ref id="scirp.47692-ref2"><label>2</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>GL&amp;#246;CKLE</surname><given-names> W.G. </given-names></name>,<name name-style="western"><surname> NONNENMACHER</surname><given-names> T.F. </given-names></name>,<etal>et al</etal>. (<year>1995</year>)<article-title>A FRACTIONAL CALCULUS APPROACH TO SELF SIMILAR PROTEIN DYNAMICS</article-title><source>. BIOPHYSICAL JOURNAL</source><volume> 68</volume>,<fpage> 46</fpage>-<lpage>53</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/S0006-3495(95)80157-8</pub-id></mixed-citation></ref><ref id="scirp.47692-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">PODLUBNY, I. (1999) FRACTIONAL DIFFERENTIAL EQUATIONS. ACADEMIC PRESS, SAN DIEGO.</mixed-citation></ref><ref id="scirp.47692-ref4"><label>4</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>HE</surname><given-names> J.H. </given-names></name>,<etal>et al</etal>. (1999)<article-title>SOME APPLICATIONS OF NONLINEAR FRACTIONAL DIFFERENTIAL EQUATIONS AND THEIR APPLICATIONS</article-title><source>. BULLETIN OF SCIENCE AND TECHNOLOGY</source><volume> 15</volume>,<fpage> 86</fpage>-<lpage>90</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.47692-ref5"><label>5</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>WANG</surname><given-names> Q. </given-names></name>,<etal>et al</etal>. (<year>2006</year>)<article-title>NUMERICAL SOLUTIONS FOR FRACTIONAL KDV-BURGERS EQUATION BY ADOMIAN DECOMPOSITION METHOD</article-title><source>. APPLIED MATHEMATICS AND COMPUTATION</source><volume> 182</volume>,<fpage> 1048</fpage>-<lpage>1055</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.AMC.2006.05.004</pub-id></mixed-citation></ref><ref id="scirp.47692-ref6"><label>6</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>RAHMAN</surname><given-names> M.</given-names></name>,<name name-style="western"><surname> MAHMOOD</surname><given-names> A. </given-names></name>,<name name-style="western"><surname> YOUNIS</surname><given-names> M. </given-names></name>,<etal>et al</etal>. (<year>2014</year>)<article-title>IMPROVED AND MORE FEASIBLE NUMERICAL METHODS FOR RIESZ SPACE FRACTIONAL PARTIAL DIFFERENTIAL EQUATIONS</article-title><source>. APPLIED MATHEMATICS AND COMPUTATION</source><volume> 237</volume>,<fpage> 264</fpage>-<lpage>273</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.AMC.2014.03.103</pub-id></mixed-citation></ref><ref id="scirp.47692-ref7"><label>7</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>LIU</surname><given-names> J. </given-names></name>,<name name-style="western"><surname> HOU</surname><given-names> G. </given-names></name>,<etal>et al</etal>. (<year>2011</year>)<article-title>NUMERICAL SOLUTIONS OF THE SPACE- AND TIME-FRACTIONAL COUPLED BURGERS EQUATIONS BY GENERALIZED DIFFERENTIAL TRANSFORM METHOD</article-title><source>. APPLIED MATHEMATICS AND COMPUTATION</source><volume> 217</volume>,<fpage> 7001</fpage>-<lpage>7008</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.AMC.2011.01.111</pub-id></mixed-citation></ref><ref id="scirp.47692-ref8"><label>8</label><mixed-citation publication-type="other" xlink:type="simple">IFTIKHAR, M., REHMAN, H.U. AND YOUNIS, M. (2013) SOLUTION OF THIRTEENTH ORDER BOUNDARY VALUE PROBLEMS BY DIFFERENTIAL TRANSFORMATION METHOD. ASIAN JOURNAL OF MATHEMATICS AND APPLICATIONS, 2014, 11 P.</mixed-citation></ref><ref id="scirp.47692-ref9"><label>9</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>WANG</surname><given-names> M.</given-names></name>,<name name-style="western"><surname> LI</surname><given-names> X. </given-names></name>,<name name-style="western"><surname> ZHANG</surname><given-names> J. </given-names></name>,<etal>et al</etal>. (<year>2008</year>)<article-title>THE  -EXPANSION METHOD AND TRAVELLING WAVE SOLTIONS OF NONLINEAR EVOLUTION EQUATIONS IN MATHEMATICAL PHYSICS</article-title><source>. PHYSICS LETTERS A</source><volume> 372</volume>,<fpage> 417</fpage>-<lpage>423</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.PHYSLETA.2007.07.051</pub-id></mixed-citation></ref><ref id="scirp.47692-ref10"><label>10</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>BIN</surname><given-names> Z. </given-names></name>,<etal>et al</etal>. (<year>2012</year>)<article-title>-EXPANSION METHOD FOR SOLVING FRACTIONAL PARTIAL DIFFERENTIAL EQUATIONS IN THE THEORY OF MATHEMATICAL PHYSICS</article-title><source>. COMMUNICATIONS IN THEORETICAL PHYSICS</source><volume> 58</volume>,<fpage> 623</fpage>-<lpage>630</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1088/0253-6102/58/5/02</pub-id></mixed-citation></ref><ref id="scirp.47692-ref11"><label>11</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>YOUNIS</surname><given-names> M. </given-names></name>,<name name-style="western"><surname> ZAFAR</surname><given-names> A. </given-names></name>,<etal>et al</etal>. (<year>2014</year>)<article-title>EXACT SOLUTION TO NONLINEAR DIFFERENTIAL EQUATIONS OF FRACTIONAL ORDER VIA  - EXPANSION METHOD</article-title><source>. APPLIED MATHEMATICS</source><volume> 5</volume>,<fpage> 1</fpage>-<lpage>6</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.4236/AM.2014.51001</pub-id></mixed-citation></ref><ref id="scirp.47692-ref12"><label>12</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>LIU</surname><given-names> S.K.</given-names></name>,<name name-style="western"><surname> FU</surname><given-names> Z.T.</given-names></name>,<name name-style="western"><surname> LIU</surname><given-names> S.D. </given-names></name>,<name name-style="western"><surname> ZHAO</surname><given-names> Q. </given-names></name>,<etal>et al</etal>. (<year>2001</year>)<article-title>JACOBI ELLIPTIC FUNCTION EXPANSION METHOD AND PERIODIC WAVE SOLUTIONS OF NONLINEAR WAVE EQUATIONS</article-title><source>. PHYSICS LETTERS A</source><volume> 289</volume>,<fpage> 69</fpage>-<lpage>74</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/S0375-9601(01)00580-1</pub-id></mixed-citation></ref><ref id="scirp.47692-ref13"><label>13</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>PARKES</surname><given-names> E.J. </given-names></name>,<name name-style="western"><surname> DUFFY</surname><given-names> B.R. </given-names></name>,<etal>et al</etal>. (<year>1996</year>)<article-title>AN AUTOMATED TANH-FUNCTION METHOD FOR FINDING SOLITARY WAVE SOLUTIONS TO NON-LINEAR EVOLUTION EQUATIONS</article-title><source>. COMPUTER PHYSICS COMMUNICATIONS</source><volume> 98</volume>,<fpage> 288</fpage>-<lpage>300</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/0010-4655(96)00104-X</pub-id></mixed-citation></ref><ref id="scirp.47692-ref14"><label>14</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>GEPREEL</surname><given-names> K.A. </given-names></name>,<etal>et al</etal>. (<year>2011</year>)<article-title>THE HOMOTOPY PERTURBATION METHOD APPLIED TO THE NONLINEAR FRACTIONAL KOLMOGOROV PETROVSKII PISKUNOV EQUATIONS</article-title><source>. APPLIED MATHEMATICS LETTERS</source><volume> 24</volume>,<fpage> 1428</fpage>-<lpage>1434</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.AML.2011.03.025</pub-id></mixed-citation></ref><ref id="scirp.47692-ref15"><label>15</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>YOUNIS</surname><given-names> M. </given-names></name>,<etal>et al</etal>. (<year>2013</year>)<article-title>THE FIRST INTEGRAL METHOD FOR TIME-SPACE FRACTIONAL DIFFERENTIAL EQUATIONS</article-title><source>. JOURNAL OF ADVANCED PHYSICS</source><volume> 2</volume>,<fpage> 220</fpage>-<lpage>223</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1166/JAP.2013.1074</pub-id></mixed-citation></ref><ref id="scirp.47692-ref16"><label>16</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>YOUNIS</surname><given-names> M. </given-names></name>,<name name-style="western"><surname> ALI</surname><given-names> S. </given-names></name>,<etal>et al</etal>. (<year>2014</year>)<article-title>NEW APPLICATIONS TO SOLITARY WAVE ANSATZ</article-title><source>. APPLIED MATHEMATICS</source><volume> 5</volume>,<fpage> 969</fpage>-<lpage>974</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.4236/AM.2014.56092</pub-id></mixed-citation></ref><ref id="scirp.47692-ref17"><label>17</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>LI</surname><given-names> Z.-B. </given-names></name>,<name name-style="western"><surname> HE</surname><given-names> J.-H. </given-names></name>,<etal>et al</etal>. (2010)<article-title>LI, Z.-B. AND HE, J.-H.  FRACTIONAL COMPLEX TRANSFORM FOR FRACTIONAL DIFFERENTIAL EQUATIONS</article-title><source>. COMPUTERS &amp; MATHEMATICS WITH APPLICATIONS</source><volume> 15</volume>,<fpage> 970</fpage>-<lpage>973</lpage>.<pub-id pub-id-type="doi"></pub-id></mixed-citation></ref><ref id="scirp.47692-ref18"><label>18</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>JAWAD</surname><given-names> A.J.M.</given-names></name>,<name name-style="western"><surname> PETKOVIC</surname><given-names> M.D. </given-names></name>,<name name-style="western"><surname> BISWAS</surname><given-names> A. </given-names></name>,<etal>et al</etal>. (<year>2010</year>)<article-title>MODIFIED SIMPLE EQUATION METHOD FOR NONLINEAR EVOLUTION EQUATIONS</article-title><source>. APPLIED MATHEMATICS AND COMPUTATION</source><volume> 217</volume>,<fpage> 869</fpage>-<lpage>877</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.AMC.2010.06.030</pub-id></mixed-citation></ref><ref id="scirp.47692-ref19"><label>19</label><mixed-citation publication-type="other" xlink:type="simple">YOUNIS, M., IFTIKHAR, M. AND REHMAN, H.U. (2014) EXACT SOLUTIONS TO THE NONLINEAR SCHRDINGER AND ECKHAUS EQUATIONS BY MODIED SIMPLE EQUATION METHOD. JOURNAL OF ADVANCED PHYSICS, (ACCEPTED).</mixed-citation></ref><ref id="scirp.47692-ref20"><label>20</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>JUMARIE</surname><given-names> G. </given-names></name>,<etal>et al</etal>. (<year>2006</year>)<article-title>MODIFIED RIEMANN-LIOUVILLE DERIVATIVE AND FRACTIONAL TAYLOR SERIES OF NONDIFFERENTIABLE FUNCTIONS FURTHER RESULTS</article-title><source>. COMPUTERS &amp; MATHEMATICS WITH APPLICATIONS</source><volume> 51</volume>,<fpage> 1367</fpage>-<lpage>1624</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.CAMWA.2006.02.001</pub-id></mixed-citation></ref><ref id="scirp.47692-ref21"><label>21</label><mixed-citation publication-type="journal" xlink:type="simple"><name name-style="western"><surname>JUMARIE</surname><given-names> G. </given-names></name>,<etal>et al</etal>. (<year>2009</year>)<article-title>LAPLACE TRANSFORM OF FRACTIONAL ORDER VIA THE MITTAG LEFFLER FUNCTION AND MODIFIED RIEMANNAN LIOUVILLE DERIVATIVE</article-title><source>. APPLIED MATHEMATICS LETTERS</source><volume> 22</volume>,<fpage> 1659</fpage>-<lpage>1664</lpage>.<pub-id pub-id-type="doi">HTTP://DX.DOI.ORG/10.1016/J.AML.2009.05.011</pub-id></mixed-citation></ref></ref-list></back></article>