<?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">AJCM</journal-id><journal-title-group><journal-title>American Journal of Computational Mathematics</journal-title></journal-title-group><issn pub-type="epub">2161-1203</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ajcm.2015.53030</article-id><article-id pub-id-type="publisher-id">AJCM-59492</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>
 
 
  Adomian Decomposition Approach to the Solution of the Burger’s Equation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>yakino</surname><given-names>P. Akpan</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>Department of Basic Science, College of Agriculture, Lafia, Nigeria</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>akpanip@yahoo.com</email></corresp></author-notes><pub-date pub-type="epub"><day>20</day><month>08</month><year>2015</year></pub-date><volume>05</volume><issue>03</issue><fpage>329</fpage><lpage>335</lpage><history><date date-type="received"><day>16</day>	<month>July</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>6</month>	<year>September</year>	</date><date date-type="accepted"><day>9</day>	<month>September</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>
 
 
  Adomian decomposition method is presented as a method for the solution of the Burger’s equation, a popular PDE model in the fluid mechanics. The method is computationally simple in application. The approximate solution is obtained by considering only the first two terms of the decomposition in this paper. Numerical experimentation shows accuracy of a minimum error of order five for various space steps and coefficient of kinematic viscosity. The method is considered high in accuracy.
 
</p></abstract><kwd-group><kwd>Adomian Decomposition</kwd><kwd> Burger’s Equation</kwd><kwd> Kinematic Viscosity</kwd><kwd> Nonlinear Operators</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Burger’s equation is a fundamental partial differential equation in fluid mechanics. It is also a very important model encountered in several areas of applied mathematics such as heat conduction, acoustic waves, gas dynamics and traffic flow [<xref ref-type="bibr" rid="scirp.59492-ref1">1</xref>] . Analytical solutions of the partial differential equations modeling physical phenomena exist only in few of the cases. Therefore the need for the construction of efficient numerical methods for the approximate solution of these models always exists. Many of the analytical solutions to the Burger’s equation involve Fourier series. According to [<xref ref-type="bibr" rid="scirp.59492-ref2">2</xref>] , the convergence of such Fourier-series based solutions is very slow. Several researchers have proposed various numerical methods for the solution of the Burger’s equation. [<xref ref-type="bibr" rid="scirp.59492-ref3">3</xref>] and [<xref ref-type="bibr" rid="scirp.59492-ref4">4</xref>] used the finite element method for the solution of the Burger’s equation. [<xref ref-type="bibr" rid="scirp.59492-ref5">5</xref>] and [<xref ref-type="bibr" rid="scirp.59492-ref6">6</xref>] used the finite difference method. [<xref ref-type="bibr" rid="scirp.59492-ref7">7</xref>] used the direct variational method while [<xref ref-type="bibr" rid="scirp.59492-ref8">8</xref>] used the projection method by B-spline.</p><p>A decomposition method which provides convergent solutions to nonlinear stochastic operator equations was developed in [<xref ref-type="bibr" rid="scirp.59492-ref9">9</xref>] . [<xref ref-type="bibr" rid="scirp.59492-ref10">10</xref>] gave proof of convergence of Adomian decomposition method when applied to differential equations. [<xref ref-type="bibr" rid="scirp.59492-ref11">11</xref>] constructed an algorithm for solving nonlinear equations based on Newton-Raphson method using Adomian decomposition approach. In an effort to extend the usefulness of Adomian’s decomposition method into other areas of mathematics, [<xref ref-type="bibr" rid="scirp.59492-ref12">12</xref>] developed a technique for calculating Adomian’s polynomials for nonlinear operators. [<xref ref-type="bibr" rid="scirp.59492-ref13">13</xref>] presented a method for the solution of homogeneous differential equations using Adomian’s decomposition without noisy terms. [<xref ref-type="bibr" rid="scirp.59492-ref14">14</xref>] extended the application of the Adomian decomposition method for the calculations of non-differential functions.</p><p>In this paper, presentation of a numerical method for the solution of the nonlinear reaction-diffusion Burger’s equation using Adomian decomposition is made. The organization of this paper is as follows: in Section 2 the theoretical approach is presented. In Section 3 the Adomian’s polynomials for the Burger’s equation are determined. In Section 4 computational results for the Burger’s equation using Adomian’s decomposition are presented while conclusion is presented in Section 5.</p></sec><sec id="s2"><title>2. Theoretical Approach</title><p>Consider the Burger’s equation</p><disp-formula id="scirp.59492-formula203"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x5.png"  xlink:type="simple"/></disp-formula><p>Subject to initial condition</p><disp-formula id="scirp.59492-formula204"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x6.png"  xlink:type="simple"/></disp-formula><p>And boundary conditions:</p><disp-formula id="scirp.59492-formula205"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x7.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59492-formula206"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x8.png"  xlink:type="simple"/></disp-formula><p>Defining the operators:</p><disp-formula id="scirp.59492-formula207"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x9.png"  xlink:type="simple"/></disp-formula><p>Equation (1) can be written as:</p><disp-formula id="scirp.59492-formula208"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x10.png"  xlink:type="simple"/></disp-formula><p>Solving Equation (6) for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x11.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x12.png" xlink:type="simple"/></inline-formula> respectively gives</p><disp-formula id="scirp.59492-formula209"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x13.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.59492-formula210"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x14.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x15.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x16.png" xlink:type="simple"/></inline-formula> are the inverse operators of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x17.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x18.png" xlink:type="simple"/></inline-formula> given respectively as:</p><disp-formula id="scirp.59492-formula211"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x19.png"  xlink:type="simple"/></disp-formula><p>Operating both sides of Equations (7) and (8) with the inverse operators (9) we obtain:</p><disp-formula id="scirp.59492-formula212"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x20.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59492-formula213"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x21.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.59492-formula214"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x22.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.59492-formula215"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x23.png"  xlink:type="simple"/></disp-formula><p>Adding Equations (10) and (11) and dividing by 2, gives the canonical form:</p><disp-formula id="scirp.59492-formula216"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x24.png"  xlink:type="simple"/></disp-formula><p>The parameterized form of (14) is</p><disp-formula id="scirp.59492-formula217"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x25.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.59492-formula218"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x26.png"  xlink:type="simple"/></disp-formula><p>According to [<xref ref-type="bibr" rid="scirp.59492-ref15">15</xref>] the parameterized decomposition forms of and N<sub>u</sub> are:</p><disp-formula id="scirp.59492-formula219"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x27.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59492-formula220"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x28.png"  xlink:type="simple"/></disp-formula><p>A<sub>n</sub> are the Adomian’s polynomials which can be generated for all types of nonlinearities [<xref ref-type="bibr" rid="scirp.59492-ref16">16</xref>] .</p><p>Substituting Equations (17) and (18) into Equation (15) gives</p><disp-formula id="scirp.59492-formula221"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x29.png"  xlink:type="simple"/></disp-formula><p>Expanding both sides of Equation (19) gives</p><disp-formula id="scirp.59492-formula222"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x30.png"  xlink:type="simple"/></disp-formula><p>By comparing coefficients of both hand sides of Equation (20), it is obtained that:</p><disp-formula id="scirp.59492-formula223"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x31.png"  xlink:type="simple"/></disp-formula><p>From which we establish the recursive relation</p><disp-formula id="scirp.59492-formula224"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x32.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. Determination of Adomian’s Polynomials</title><p>The Adomian’s polynomials, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x33.png" xlink:type="simple"/></inline-formula>are defined in such a way that</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x34.png" xlink:type="simple"/></inline-formula>[<xref ref-type="bibr" rid="scirp.59492-ref17">17</xref>]</p><p>Substituting Equation (17) into Equation (18) and expanding the RHS gives</p><disp-formula id="scirp.59492-formula225"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x35.png"  xlink:type="simple"/></disp-formula><p>From Equation (22), we establish that the Adomian’s polynomials have the following forms:</p><disp-formula id="scirp.59492-formula226"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x36.png"  xlink:type="simple"/></disp-formula><p>The Adomian’s polynomials for Equation (1) are obtained from the recurrent relation</p><disp-formula id="scirp.59492-formula227"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/11-1100460x37.png"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Numerical Experiment</title><p>We present numerical results to illustrate the effectiveness of the proposed method. Consider Burger’s Equation (1) with the following initial and boundary conditions.</p><disp-formula id="scirp.59492-formula228"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x38.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.59492-formula229"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x39.png"  xlink:type="simple"/></disp-formula><p>The exact solution of Equation (1) with the above conditions was given in [<xref ref-type="bibr" rid="scirp.59492-ref1">1</xref>] as</p><disp-formula id="scirp.59492-formula230"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x40.png"  xlink:type="simple"/></disp-formula>Computations of Absolute and Relative Errors<p>Absolute errors of the method were computed by use of the formula:</p><disp-formula id="scirp.59492-formula231"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x41.png"  xlink:type="simple"/></disp-formula><p>where the numerical solution at the grid point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x42.png" xlink:type="simple"/></inline-formula> is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x43.png" xlink:type="simple"/></inline-formula>, and the exact solution at the same grid point is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x44.png" xlink:type="simple"/></inline-formula>.</p><p>Relative errors were computed by use of the formula:</p><disp-formula id="scirp.59492-formula232"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x45.png"  xlink:type="simple"/></disp-formula><p>where the numerical solution at the grid point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x46.png" xlink:type="simple"/></inline-formula> is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x47.png" xlink:type="simple"/></inline-formula>, and the exact solution at the same grid point is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x48.png" xlink:type="simple"/></inline-formula>.</p><p><xref ref-type="fig" rid="fig1">Figure 1</xref> is a 3 dimensional plot of the surface <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x49.png" xlink:type="simple"/></inline-formula> while <xref ref-type="fig" rid="fig2">Figure 2</xref> is a 3 dimensional plot of the surface <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x52.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.59492-formula233"><graphic  xlink:href="http://html.scirp.org/file/11-1100460x55.png"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, Adomian decomposition method is used to solve the burger’s equation numerically. From <xref ref-type="table" rid="table1">Table 1</xref> and <xref ref-type="table" rid="table2">Table 2</xref>, this method is considered to give accurate results for specified values of the parameter, ε. We considered the first two terms of the decomposition to make the approximate solution. Accuracy of the method</p><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> A 3 dimensional plot of the surface<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x57.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-1100460x56.png"/></fig><fig id="fig2"  position="float"><label><xref ref-type="fig" rid="fig2">Figure 2</xref></label><caption><title> A 3 dimensional plot of the surface<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/11-1100460x59.png" xlink:type="simple"/></inline-formula></title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/11-1100460x58.png"/></fig><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Approximate solutions by Adomian’s decomposition, errors and relative errors for t = 0.2, e = 0.001, a = 2</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >x</th><th align="center" valign="middle" >Adomian</th><th align="center" valign="middle" >Theoretical solution</th><th align="center" valign="middle" >Error</th><th align="center" valign="middle" >Relative Errors</th></tr></thead><tr><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >0.0006610924400</td><td align="center" valign="middle" >0.0003891849100</td><td align="center" valign="middle" >2.719075297 &#215; 10<sup>−4 </sup></td><td align="center" valign="middle" >2.718017485 &#215; 10<sup>−4 </sup></td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.0013184569550</td><td align="center" valign="middle" >0.0008129882596</td><td align="center" valign="middle" >5.054686954 &#215; 10<sup>−4 </sup></td><td align="center" valign="middle" >5.050580892 &#215; 10<sup>−4 </sup></td></tr><tr><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >0.001968724990</td><td align="center" valign="middle" >0.0013210998120</td><td align="center" valign="middle" >6.47625178 &#215; 10<sup>−4 </sup></td><td align="center" valign="middle" >6.467707292 &#215;10<sup>−4 </sup></td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.002596743099</td><td align="center" valign="middle" >0.0020106848070</td><td align="center" valign="middle" >5.86058292 &#215; 10<sup>−4 </sup></td><td align="center" valign="middle" >5.84882278 &#215; 10<sup>−4 </sup></td></tr><tr><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >0.0031486447293</td><td align="center" valign="middle" >0.0031366545250</td><td align="center" valign="middle" >1.9922768 &#215; 10<sup>−5 </sup></td><td align="center" valign="middle" >1.986047255 &#215; 10<sup>−5 </sup></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.003546100003</td><td align="center" valign="middle" >0.005799752849</td><td align="center" valign="middle" >2.253652846 &#215; 10<sup>−3 </sup></td><td align="center" valign="middle" >2.240657585 &#215; 10<sup>−3 </sup></td></tr><tr><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >0.003616277199</td><td align="center" valign="middle" >0.03291862860</td><td align="center" valign="middle" >2.930235148 &#215; 10<sup>−2 </sup></td><td align="center" valign="middle" >2.836849937 &#215; 10<sup>−2 </sup></td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.003425426033</td><td align="center" valign="middle" >−0.006782588856</td><td align="center" valign="middle" >1.020801489 &#215; 10<sup>−2 </sup></td><td align="center" valign="middle" >1.027772447 &#215; 10<sup>−2 </sup></td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Approximate solutions by Adomian’s decomposition, errors and relative errors for t = 0.05, e = 0.01, a = 2</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >x</th><th align="center" valign="middle" >Adomian</th><th align="center" valign="middle" >Theoretical Solution</th><th align="center" valign="middle" >Error</th><th align="center" valign="middle" >Relative Errors</th></tr></thead><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.01342133395</td><td align="center" valign="middle" >0.008119261273</td><td align="center" valign="middle" >5.302072677 &#215; 10<sup>−3 </sup></td><td align="center" valign="middle" >5.259370475 &#215; 10<sup>−3 </sup></td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.02618512105</td><td align="center" valign="middle" >0.02006671613</td><td align="center" valign="middle" >6.11840492 &#215; 10<sup>−3 </sup></td><td align="center" valign="middle" >5.998043877 &#215; 10<sup>−3 </sup></td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.03577004231</td><td align="center" valign="middle" >0.05766474009</td><td align="center" valign="middle" >2.189469778 &#215; 10<sup>−2 </sup></td><td align="center" valign="middle" >2.070098109 &#215; 10<sup>−2 </sup></td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.03132012403</td><td align="center" valign="middle" >−0.06901554553</td><td align="center" valign="middle" >1.003356696 &#215; 10<sup>−1 </sup></td><td align="center" valign="middle" >1.077737325 &#215; 10<sup>−1 </sup></td></tr></tbody></table></table-wrap><p>can be improved by considering more terms in the solution approximation. 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