<?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.2016.717172</article-id><article-id pub-id-type="publisher-id">AM-72080</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Zhou’s Method for Solving the Euler Equidimensional Equation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Pedro</surname><given-names>Pablo Cárdenas Alzate</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>Jhon</surname><given-names>Jairo León Salazar</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>Carlos</surname><given-names>Alberto Rodríguez Varela</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics and GEDNOL, Universidad Tecnológica de Pereira, Pereira, Colombia</addr-line></aff><aff id="aff2"><addr-line>Department of Mathematics, Universidad Tecnológica de Pereira, Pereira, Colombia</addr-line></aff><pub-date pub-type="epub"><day>14</day><month>11</month><year>2016</year></pub-date><volume>07</volume><issue>17</issue><fpage>2165</fpage><lpage>2173</lpage><history><date date-type="received"><day>September</day>	<month>15,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>November</month>	<year>14,</year>	</date><date date-type="accepted"><day>November</day>	<month>17,</month>	<year>2016</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 work, we apply the Zhou’s method [1] or differential transformation method (DTM) for solving the Euler equidimensional equation. The Zhou’s method may be considered as alternative and efficient for finding the approximate solutions of initial values problems. We prove superiority of this method by applying them on the some Euler type equation, in this case of order 2 and 3 [2]. The power series solution of the reduced equation transforms into an approximate implicit solution of the original equations. The results agreed with the exact solution obtained via transformation to a constant coefficient equation.
 
</p></abstract><kwd-group><kwd>Zhou’s Method</kwd><kwd> Equidimensional Equation</kwd><kwd> Euler Equation</kwd><kwd> DTM</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We know that when the coefficients <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x2.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x3.png" xlink:type="simple"/></inline-formula> are analytic functions on a given domain, then the equation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x4.png" xlink:type="simple"/></inline-formula> has analytic fundamental solution. We want to study equations with coefficients p and q having singularities, for this reason we study in this paper with one of the simplest cases, Euler’s equidimen- sional equation. This is an important problem because many differential equations in physical sciences have coefficients with singularities [<xref ref-type="bibr" rid="scirp.72080-ref3">3</xref>] . One of the special features of the equidimensional equation is that order of each derivative is equal to the power of the independent variable. This means that this type of equations can be reduced to linear equation with constant coefficient by using a change of the form<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x5.png" xlink:type="simple"/></inline-formula>.</p><p>Many numerical methods were developed for this type of equations, specifically on Euler’s equations such that Laplace transform method and Adomian method [<xref ref-type="bibr" rid="scirp.72080-ref4">4</xref>] . The method proposed in this paper was first established by Zhou to solve problems in electric circuits analysis. In this work, the differential transformation method is applied to solver the Euler equidimensional equations and to illustrate this method, several equations of this type are solved [<xref ref-type="bibr" rid="scirp.72080-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.72080-ref6">6</xref>] .</p></sec><sec id="s2"><title>2. The Euler Equidimensional Equation</title><p>A Euler equidimensional equation is a differential equation of the form</p><disp-formula id="scirp.72080-formula348"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x6.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x7.png" xlink:type="simple"/></inline-formula> are constants and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x8.png" xlink:type="simple"/></inline-formula> is an n-th derivative of the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x9.png" xlink:type="simple"/></inline-formula></p><p>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x10.png" xlink:type="simple"/></inline-formula> is a continuous function.</p><p>Now, we consider a second order differential equation (homogeneous Euler equidi- mensional) of the form</p><disp-formula id="scirp.72080-formula349"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x11.png"  xlink:type="simple"/></disp-formula><p>The solution can be obtained by using the change of variables</p><disp-formula id="scirp.72080-formula350"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x12.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x13.png" xlink:type="simple"/></inline-formula>. In fact, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x14.png" xlink:type="simple"/></inline-formula>, we introduce<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x15.png" xlink:type="simple"/></inline-formula>, therefore<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x16.png" xlink:type="simple"/></inline-formula>. Then, the</p><p>first and second derivatives of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x17.png" xlink:type="simple"/></inline-formula> are related by the chain rule,</p><disp-formula id="scirp.72080-formula351"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x18.png"  xlink:type="simple"/></disp-formula><p>Now, substituting (4) in (2) yields a second order differential equation with constant coefficients, i.e.,</p><disp-formula id="scirp.72080-formula352"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x19.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula353"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x20.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula354"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x21.png"  xlink:type="simple"/></disp-formula><p>Equation (5) can be solved using the characteristic polynomial</p><disp-formula id="scirp.72080-formula355"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x22.png"  xlink:type="simple"/></disp-formula><p>where roots are <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x23.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x24.png" xlink:type="simple"/></inline-formula> which give the general solution but depending on the type of roots it has, i.e.,</p><p>a) If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x25.png" xlink:type="simple"/></inline-formula>, real or complex, then the general solution of the Equation (2) is given by</p><disp-formula id="scirp.72080-formula356"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x26.png"  xlink:type="simple"/></disp-formula><p>b) If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x27.png" xlink:type="simple"/></inline-formula>, then the general solution of the Equation (2) is given by</p><disp-formula id="scirp.72080-formula357"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x28.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. The Zhou’s Method or DTM</title><p>Differential transformation method (DTM) of the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x29.png" xlink:type="simple"/></inline-formula> is defined as</p><disp-formula id="scirp.72080-formula358"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x30.png"  xlink:type="simple"/></disp-formula><p>In (7), we have that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x31.png" xlink:type="simple"/></inline-formula> is the original function and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x32.png" xlink:type="simple"/></inline-formula> is the transformed function. The inverse differential transformation is defined as</p><disp-formula id="scirp.72080-formula359"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x33.png"  xlink:type="simple"/></disp-formula><p>but in real applications, function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x34.png" xlink:type="simple"/></inline-formula> is expressed by a finite series and Equation (8) can be written as</p><disp-formula id="scirp.72080-formula360"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x35.png"  xlink:type="simple"/></disp-formula><p>which implies that</p><disp-formula id="scirp.72080-formula361"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x36.png"  xlink:type="simple"/></disp-formula><p>is negligibly small where n is decided by the convergence of natural frequency in this study.</p><p>The following theorems that can be deduced from Equations (7) and (9) and the proofs are available in [<xref ref-type="bibr" rid="scirp.72080-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.72080-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.72080-ref6">6</xref>] .</p><p>Theorem 1 If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x37.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x38.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 2 If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x39.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x40.png" xlink:type="simple"/></inline-formula> with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x40.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x41.png" xlink:type="simple"/></inline-formula> constant.</p><p>Theorem 3 If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x42.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x43.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 4 If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x44.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x45.png" xlink:type="simple"/></inline-formula>.</p><p>Theorem 5 If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x46.png" xlink:type="simple"/></inline-formula>, then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x47.png" xlink:type="simple"/></inline-formula>, where</p><disp-formula id="scirp.72080-formula362"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x48.png"  xlink:type="simple"/></disp-formula><p>Theorem 6 (C&#225;rdenas, P). If<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x49.png" xlink:type="simple"/></inline-formula>, then</p><disp-formula id="scirp.72080-formula363"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x50.png"  xlink:type="simple"/></disp-formula><p>with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x51.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Numerical Results</title><p>To illustrate the ability of the Zhou’s method [<xref ref-type="bibr" rid="scirp.72080-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.72080-ref7">7</xref>] for the Euler equidimensional equation, the next problem is provided and the results reveal that this method is very effective.</p><p>Example 1 (Homogeneous case). To begin, we consider the initial value problem</p><disp-formula id="scirp.72080-formula364"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x52.png"  xlink:type="simple"/></disp-formula><p>Using the substitution (3) and (4), the IVP (10) is transformed to a second order differential equation with constant coefficients, i.e.,</p><disp-formula id="scirp.72080-formula365"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x53.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula366"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x54.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula367"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x55.png"  xlink:type="simple"/></disp-formula><p>Now, of the initial conditions we have that as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x56.png" xlink:type="simple"/></inline-formula>, then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x57.png" xlink:type="simple"/></inline-formula> and therefore <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x58.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x58.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x59.png" xlink:type="simple"/></inline-formula>. So, the new IVP is given by</p><disp-formula id="scirp.72080-formula368"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x60.png"  xlink:type="simple"/></disp-formula><p>The exact solution of the problem (12) is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x61.png" xlink:type="simple"/></inline-formula>. Taking the differential transformation of this problem we obtain</p><disp-formula id="scirp.72080-formula369"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x62.png"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.72080-formula370"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x63.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x64.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x64.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x65.png" xlink:type="simple"/></inline-formula>. Therefore, the recurrence Equation (13) gives:</p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x66.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula371"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x67.png"  xlink:type="simple"/></disp-formula><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x68.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula372"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x69.png"  xlink:type="simple"/></disp-formula><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x70.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula373"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x71.png"  xlink:type="simple"/></disp-formula><p>Therefore, using (9), the closed form of the solution can be easily written as</p><disp-formula id="scirp.72080-formula374"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x72.png"  xlink:type="simple"/></disp-formula><p>but since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x73.png" xlink:type="simple"/></inline-formula>, then we obtain (see <xref ref-type="fig" rid="fig1">Figure 1</xref>)</p><disp-formula id="scirp.72080-formula375"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x74.png"  xlink:type="simple"/></disp-formula><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The Zhou’s method vs. exact solution.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7403392x75.png"/></fig></fig-group><p>Example 2 (Non-homogeneous case). We consider the following IVP</p><disp-formula id="scirp.72080-formula376"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x76.png"  xlink:type="simple"/></disp-formula><p>Then, problem (15) is transformed to a second order differential equation with con- stant coefficient by using (3) and (4), i.e.,</p><disp-formula id="scirp.72080-formula377"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula378"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x78.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula379"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x79.png"  xlink:type="simple"/></disp-formula><p>We know that of the initial conditions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x80.png" xlink:type="simple"/></inline-formula> and therefore<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x81.png" xlink:type="simple"/></inline-formula>, so we obtain <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x82.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x82.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x83.png" xlink:type="simple"/></inline-formula>. Then, the IVP is given by</p><disp-formula id="scirp.72080-formula380"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x84.png"  xlink:type="simple"/></disp-formula><p>The exact solution of the problem (15) is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x85.png" xlink:type="simple"/></inline-formula>. Now, the DTM of (17) is</p><disp-formula id="scirp.72080-formula381"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x86.png"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.72080-formula382"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x87.png"  xlink:type="simple"/></disp-formula><p>with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x88.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x88.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x89.png" xlink:type="simple"/></inline-formula>. So, the recurrence Equation (18) gives:</p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x90.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula383"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x91.png"  xlink:type="simple"/></disp-formula><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x92.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula384"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x93.png"  xlink:type="simple"/></disp-formula><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x94.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula385"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x95.png"  xlink:type="simple"/></disp-formula><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x96.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula386"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x97.png"  xlink:type="simple"/></disp-formula><p>Therefore, using (9), the closed form of the solution can be easily written as</p><disp-formula id="scirp.72080-formula387"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x98.png"  xlink:type="simple"/></disp-formula><p>But since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x99.png" xlink:type="simple"/></inline-formula>, then we obtain (see <xref ref-type="fig" rid="fig2">Figure 2</xref>)</p><disp-formula id="scirp.72080-formula388"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x100.png"  xlink:type="simple"/></disp-formula><p>Example 3 (Third order Euler’s equation). Consider the following IVP</p><disp-formula id="scirp.72080-formula389"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x101.png"  xlink:type="simple"/></disp-formula><p>Now, to find <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x102.png" xlink:type="simple"/></inline-formula> we use the chain rule. In fact we obtain</p><fig-group id="fig2"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> The Zhou’s method vs. exact solution.</title></caption><fig id ="fig2_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7403392x103.png"/></fig></fig-group><disp-formula id="scirp.72080-formula390"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x104.png"  xlink:type="simple"/></disp-formula><p>Therefore, using (3), (4) and (21) we have</p><disp-formula id="scirp.72080-formula391"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x105.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula392"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x106.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72080-formula393"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x107.png"  xlink:type="simple"/></disp-formula><p>Now, as in the previous example <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x108.png" xlink:type="simple"/></inline-formula> and then<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x109.png" xlink:type="simple"/></inline-formula>. So, the new initial con- ditions are given by <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x110.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x108.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x109.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x110.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x111.png" xlink:type="simple"/></inline-formula>. Using (7) we find that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x112.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x113.png" xlink:type="simple"/></inline-formula>. Therefore, we obtain the IVP</p><disp-formula id="scirp.72080-formula394"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x114.png"  xlink:type="simple"/></disp-formula><p>Applying DTM to (23) we obtain</p><disp-formula id="scirp.72080-formula395"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x115.png"  xlink:type="simple"/></disp-formula><p>or</p><disp-formula id="scirp.72080-formula396"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x116.png"  xlink:type="simple"/></disp-formula><p>So, the recurrence equation (24) gives:</p><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x117.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula397"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x118.png"  xlink:type="simple"/></disp-formula><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x119.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula398"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x120.png"  xlink:type="simple"/></disp-formula><p>・ <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x121.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.72080-formula399"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x122.png"  xlink:type="simple"/></disp-formula><p>Therefore, using (9), the closed form of the solution can be easily written as</p><fig-group id="fig3"><label><xref ref-type="fig" rid="fig3">Figure 3</xref></label><caption><title> The Zhou’s method vs. exact solution.</title></caption><fig id ="fig3_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/7-7403392x123.png"/></fig></fig-group><disp-formula id="scirp.72080-formula400"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/7-7403392x124.png"  xlink:type="simple"/></disp-formula><p>But since<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/7-7403392x125.png" xlink:type="simple"/></inline-formula>, then we obtain (see <xref ref-type="fig" rid="fig3">Figure 3</xref>)</p><disp-formula id="scirp.72080-formula401"><graphic  xlink:href="http://html.scirp.org/file/7-7403392x126.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, we presented the definition and handling of one-dimensional differential transformation method or Zhou’s method. Using the substitutions (3) and (4), Euler’s equidimensional equations were transformed to a second and third order differential equations with constant coefficients, next using DTM these equations were transformed into algebraic equations (iterative equations). The new scheme obtained by using the Zhou’s method yields an analytical solution in the form of a rapidly convergent series. This method makes the solution procedure much more attractive. The figures [<xref ref-type="bibr" rid="scirp.72080-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.72080-ref5">5</xref>] and [<xref ref-type="bibr" rid="scirp.72080-ref6">6</xref>] clearly show the high efficiency of DTM with the three examples proposed.</p></sec><sec id="s6"><title>Acknowledgements</title><p>Foremost, we would like to express my sincere gratitude to the Department of Mathematics of the Universidad Tecnol&#243;gica de Pereira and group GEDNOL for the support in this work. In the same way, we would like to express sincere thanks to the anonymous reviewers for their positive and constructive comments towards the improvement of the article.</p></sec><sec id="s7"><title>Cite this paper</title><p>C&#225;rdenas Alzate, P.P., Salazar, J.J.L. and Varela, C.A.R. (2016) The Zhou’s Method for Solving the Euler Equidimensional Equation. Applied Mathematics, 7, 2165-2173. http://dx.doi.org/10.4236/am.2016.717172</p></sec></body><back><ref-list><title>References</title><ref id="scirp.72080-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Zhou, J.K. (1986) Differential Transformation and Its Applications for Electrical Circuits. Huazhong University Press, Wuhan.</mixed-citation></ref><ref id="scirp.72080-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Odibat, Z. (2008) Differential Transform Method for Solving Volterra Integral Equations with Separable Kernels. Mathematical and Computer Modelling, 48, 1144-1146.  
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