<?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.2016.711107</article-id><article-id pub-id-type="publisher-id">AM-68152</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>
 
 
  Numerical Solutions of a Generalized Nth Order Boundary Value Problems Using Power Series Approximation Method
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Ignatius</surname><given-names>N. Njoseh</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>Ebimene</surname><given-names>J. Mamadu</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>Department of Mathematics, University of Ilorin, Ilorin, Nigeria</addr-line></aff><aff id="aff1"><addr-line>Department of Mathematics and Computer Science, Delta State University, Abraka, Nigeria</addr-line></aff><pub-date pub-type="epub"><day>11</day><month>07</month><year>2016</year></pub-date><volume>07</volume><issue>11</issue><fpage>1215</fpage><lpage>1224</lpage><history><date date-type="received"><day>6</day>	<month>May</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>8</month>	<year>July</year>	</date><date date-type="accepted"><day>11</day>	<month>July</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 paper, a new approach called Power Series Approximation Method (PSAM) is developed for the numerical solution of a generalized linear and non-linear higher order Boundary Value Problems (BVPs). The proposed method is efficient and effective on the experimentation on some selected thirteen-order, twelve-order and ten-order boundary value problems as compared with the analytic solutions and other existing methods such as the Homotopy Perturbation Method (HPM) and Variational Iteration Method (VIM) available in the literature. A convergence analysis of PSAM is also provided.
 
</p></abstract><kwd-group><kwd>Power Series</kwd><kwd> Linear and Nonlinear Problems</kwd><kwd> Boundary Value Problem (BVP)</kwd><kwd>  Numerical Simulation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Higher order boundary value problems in linear and non-linear form have been a major concern in recent years. This is due to its applicability in many areas of Mathematical Physics and other sciences in its precise analysis of nonlinear phenomena such as computation of radiowave attenuation in the atmosphere, interface conditions determination in electromagnetic field, potential theory and determination of wave nodes in wave propagation. Most conventional analytic methods for higher order boundary value problems are prone to rounding-off and computation errors. As a result, the analytics methods are less dependent in seeking the solution of higher order boundary values problems in most cases, especially the non-linear type. Thus, numerical methods have gained momentum in seeking the solution of higher order boundary value problems.</p><p>Over the years, several numerical techniques have been developed, such as the Variational Iteration Method (VIM) [<xref ref-type="bibr" rid="scirp.68152-ref1">1</xref>] , Homotopy Perturbation Method (HPM) [<xref ref-type="bibr" rid="scirp.68152-ref2">2</xref>] , Spline-Collocation Approximations Method (SCAM) [<xref ref-type="bibr" rid="scirp.68152-ref3">3</xref>] , Spline Method [<xref ref-type="bibr" rid="scirp.68152-ref4">4</xref>] , etc. that possess an elaborate procedure and structurally complex, which nevertheless yields efficient results. Siddiqi and Iftikhar [<xref ref-type="bibr" rid="scirp.68152-ref5">5</xref>] worked on a numerical solution of higher order boundary value problems. Also, Siddiqi and Iftikhar [<xref ref-type="bibr" rid="scirp.68152-ref6">6</xref>] adopted the technique of variation of parameter methods for the solution of seventh order boundary value problems. Iftikhar et al. [<xref ref-type="bibr" rid="scirp.68152-ref7">7</xref>] solved the thirteenth order value problems by Differential transform method. Akram and Rehman [<xref ref-type="bibr" rid="scirp.68152-ref8">8</xref>] presented a numerical solution of eighth order boundary value problems in reproducing kernel space. Wu et al. [<xref ref-type="bibr" rid="scirp.68152-ref9">9</xref>] presented a precise and rigorous work on nonlinear functional analysis of boundary value problems: novel theory, methods and applications. Mamadu and Njoseh [<xref ref-type="bibr" rid="scirp.68152-ref10">10</xref>] have proposed a method which efficiently finds exact solutions and is used to solve linear Volterra integral equations.</p><p>In this present work, the Power Series Approximation Method (PSAM) is a new approach developed for the numerical solution of a generalized Nth order boundary value problems. The proposed method is structurally simple with well posed Mathematical formulae. It involves transforming the given boundary value problems into system of ODEs together with the boundary conditions prescribed. Thereafter, the coefficients of the power series solution are uniquely obtained with a well posed recurrence relation along the boundary<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x6.png" xlink:type="simple"/></inline-formula>, which leads to the solution. The unknown parameters in the solution are determined at the other boundary<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x7.png" xlink:type="simple"/></inline-formula>. This finally leads to a system of algebraic equations, which on solving yields the required approximate series solution. The method is accurate and efficient in obtaining the approximate solutions of linear and non-linear boundary value problems. The method requires no discretization and linearization or perturbation. Also, computational and rounding-off errors are avoided. The method has an excellent rate of convergence as compared with existing methods in [<xref ref-type="bibr" rid="scirp.68152-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.68152-ref2">2</xref>] and the exact solutions available in the literature.</p><p>The rest of this paper will be organized as follows: Section 2 of this work give detailed Mathematical formulation of Nth order BVPs using PSAM. Section 3 presents the error analysis and convergence theorem of the method. Section 4 offers numerical stimulation of the method on some selected thirteen-order, twelve-order and ten-order boundary value problems. Finally, the conclusion is presented in Section 5.</p></sec><sec id="s2"><title>2. Power Series Approximation Method (PSAM)</title><p>We consider the Nth order BVP of the form</p><disp-formula id="scirp.68152-formula91"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x8.png"  xlink:type="simple"/></disp-formula><p>with the boundary conditions</p><disp-formula id="scirp.68152-formula92"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x9.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula93"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x10.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x11.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x12.png" xlink:type="simple"/></inline-formula> are assumed real and continuous on<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x13.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x14.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x15.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x16.png" xlink:type="simple"/></inline-formula> are finite real constants.</p><p>The given nth order BVP (1), (2) and (3) are transformed to systems of ODEs such that we have</p><disp-formula id="scirp.68152-formula94"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x17.png"  xlink:type="simple"/></disp-formula><p>with the boundary conditions</p><disp-formula id="scirp.68152-formula95"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x18.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.68152-formula96"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x19.png"  xlink:type="simple"/></disp-formula><p>Let the series approximation of (1), (2) and (3) be given as</p><disp-formula id="scirp.68152-formula97"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x20.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x21.png" xlink:type="simple"/></inline-formula> are unknown constants to be determined and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x22.png" xlink:type="simple"/></inline-formula>.</p><p>Now, we estimate the unknown constants <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x23.png" xlink:type="simple"/></inline-formula> at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x24.png" xlink:type="simple"/></inline-formula> by substituting (7) in (4) successively, which is as follows:</p><p>We consider the first derivative of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x25.png" xlink:type="simple"/></inline-formula> wrt to x as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x26.png" xlink:type="simple"/></inline-formula>, i.e.,</p><disp-formula id="scirp.68152-formula98"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x27.png"  xlink:type="simple"/></disp-formula><p>At <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x28.png" xlink:type="simple"/></inline-formula> we have,</p><disp-formula id="scirp.68152-formula99"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x29.png"  xlink:type="simple"/></disp-formula><p>Thus (8) becomes</p><disp-formula id="scirp.68152-formula100"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x30.png"  xlink:type="simple"/></disp-formula><p>Next: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x31.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68152-formula101"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x32.png"  xlink:type="simple"/></disp-formula><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x33.png" xlink:type="simple"/></inline-formula>we obtain,</p><disp-formula id="scirp.68152-formula102"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x34.png"  xlink:type="simple"/></disp-formula><p>Thus (11) becomes</p><disp-formula id="scirp.68152-formula103"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x35.png"  xlink:type="simple"/></disp-formula><p>Carrying on the above sequential approach to the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x36.png" xlink:type="simple"/></inline-formula> order we obtain the following recursive formulae at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x37.png" xlink:type="simple"/></inline-formula>,</p><disp-formula id="scirp.68152-formula104"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x38.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula105"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x39.png"  xlink:type="simple"/></disp-formula><p>Here, the choice of N is equivalent to the order of the BVP considered.</p></sec><sec id="s3"><title>3. Error Analysis and Convergence Theorem</title><p>An error estimate for the approximate solution (7) of (1), (2) and (3) is obtained here.</p><p>Let</p><disp-formula id="scirp.68152-formula106"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x40.png"  xlink:type="simple"/></disp-formula><p>as the error function of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x41.png" xlink:type="simple"/></inline-formula> to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x42.png" xlink:type="simple"/></inline-formula>; where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x42.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x43.png" xlink:type="simple"/></inline-formula> is the exact solution of (1), (2) and (3).</p><p>Hence, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x44.png" xlink:type="simple"/></inline-formula>satisfies the following problems:</p><disp-formula id="scirp.68152-formula107"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x45.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula108"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x46.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula109"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x47.png"  xlink:type="simple"/></disp-formula><p>The perturbation term <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x48.png" xlink:type="simple"/></inline-formula> can be obtained by substituting the computed solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x49.png" xlink:type="simple"/></inline-formula> to obtain</p><disp-formula id="scirp.68152-formula110"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x50.png"  xlink:type="simple"/></disp-formula><p>We then transform (16), (17) and (18) into systems of ordinary differential equations and proceed to find an approximate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x51.png" xlink:type="simple"/></inline-formula> to the error function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x51.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x52.png" xlink:type="simple"/></inline-formula> in the same way as we did before for the solution of the problem (1), (2) and (3).</p><p>Thus, the error function satisfies the problem</p><disp-formula id="scirp.68152-formula111"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x53.png"  xlink:type="simple"/></disp-formula><p>with the homogeneous conditions</p><disp-formula id="scirp.68152-formula112"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x54.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula113"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x55.png"  xlink:type="simple"/></disp-formula><sec id="s3_1"><title>3.1. Convergence Theorem</title><p>We now prove that if the solution series by PSAM is convergent, it must be an exact solution by increasing the order of approximation.</p><p>Theorem 1:</p><p>If the solution series <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x56.png" xlink:type="simple"/></inline-formula> converges it must be an exact solution by increasing the order of approximation.</p><p>Proof:</p><p>Let the series <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x57.png" xlink:type="simple"/></inline-formula> be convergent. Then</p><disp-formula id="scirp.68152-formula114"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x58.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula115"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x59.png"  xlink:type="simple"/></disp-formula><p>We have</p><disp-formula id="scirp.68152-formula116"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x60.png"  xlink:type="simple"/></disp-formula><p>Using Equation (23),</p><disp-formula id="scirp.68152-formula117"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x61.png"  xlink:type="simple"/></disp-formula><p>Using Equation (14),</p><disp-formula id="scirp.68152-formula118"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x62.png"  xlink:type="simple"/></disp-formula><p>Since <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x63.png" xlink:type="simple"/></inline-formula> in Equation (27), we have</p><disp-formula id="scirp.68152-formula119"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x64.png"  xlink:type="simple"/></disp-formula><p>If the value of N is so large or approaches infinity as in (14) and (15),</p><disp-formula id="scirp.68152-formula120"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x65.png"  xlink:type="simple"/></disp-formula><p>and this completes the proof.</p></sec></sec><sec id="s4"><title>4. Numerical Examples</title><p>To implement the method developed, three examples are considered.</p><p>Example 1</p><p>Consider the following thirteenth-order problem [<xref ref-type="bibr" rid="scirp.68152-ref1">1</xref>]</p><disp-formula id="scirp.68152-formula121"><label>, (29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x66.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula122"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x67.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula123"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x68.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula124"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x69.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula125"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x70.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula126"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x71.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula127"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x72.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula128"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x73.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula129"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x74.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula130"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula131"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula132"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x77.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula133"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x78.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula134"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x79.png"  xlink:type="simple"/></disp-formula><p>The exact solution is</p><disp-formula id="scirp.68152-formula135"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x80.png"  xlink:type="simple"/></disp-formula><p>The given 13th order BVP (29) are transformed to systems of ODEs such that we have</p><disp-formula id="scirp.68152-formula136"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x81.png"  xlink:type="simple"/></disp-formula><p>with the boundary conditions at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x82.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68152-formula137"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x83.png"  xlink:type="simple"/></disp-formula><p>The series approximation of (29) is given as Equation (7)</p><p>where the unknown constants <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x84.png" xlink:type="simple"/></inline-formula> are uniquely determined by Equation (14).</p><p>Since, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x85.png" xlink:type="simple"/></inline-formula>, we have Equation (14) as</p><disp-formula id="scirp.68152-formula138"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x86.png"  xlink:type="simple"/></disp-formula><p>Using Equation (30) for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x87.png" xlink:type="simple"/></inline-formula>, we have the following:</p><disp-formula id="scirp.68152-formula139"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x88.png"  xlink:type="simple"/></disp-formula><p>Substituting (31) into Equation (7) for N = 0 (1) 11 we obtain</p><disp-formula id="scirp.68152-formula140"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x89.png"  xlink:type="simple"/></disp-formula><p>Using boundary condition at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x90.png" xlink:type="simple"/></inline-formula> in Equation (32) we obtain the values of a, b, c, d and e, as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x91.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x92.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x93.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x94.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x90.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x91.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x92.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x93.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x94.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x95.png" xlink:type="simple"/></inline-formula>.</p><p>The above values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x96.png" xlink:type="simple"/></inline-formula> and e coincide with the results in [<xref ref-type="bibr" rid="scirp.68152-ref1">1</xref>] , where Variational Iteration Method is used for the same problem considered.</p><p>Thus, the final approximation solution of BVP (29) can be written as</p><disp-formula id="scirp.68152-formula141"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x97.png"  xlink:type="simple"/></disp-formula><p>The comparison of the approximate solution of example 1 obtained with the help of PSAM and the approximate solution using VIM obtained in [<xref ref-type="bibr" rid="scirp.68152-ref1">1</xref>] is given in <xref ref-type="table" rid="table1">Table 1</xref>. From the numerical results, it is clear that the PSAM is more efficient and accurate. By increasing the order of approximation more accuracy can be obtained.</p><p>Example 2</p><p>Consider the following linear tenth-order problem [<xref ref-type="bibr" rid="scirp.68152-ref2">2</xref>]</p><disp-formula id="scirp.68152-formula142"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x98.png"  xlink:type="simple"/></disp-formula><p>with the following boundary conditions</p><disp-formula id="scirp.68152-formula143"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x99.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula144"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x100.png"  xlink:type="simple"/></disp-formula><p>The exact solution is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x101.png" xlink:type="simple"/></inline-formula>.</p><p>The given 10th order BVP (33) is transformed to systems of ODEs such that we have</p><disp-formula id="scirp.68152-formula145"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x102.png"  xlink:type="simple"/></disp-formula><p>with the boundary conditions at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x103.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68152-formula146"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x104.png"  xlink:type="simple"/></disp-formula><p>Since, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x105.png" xlink:type="simple"/></inline-formula>, we have Equation (14) as</p><disp-formula id="scirp.68152-formula147"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x106.png"  xlink:type="simple"/></disp-formula><p>Hence for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x107.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.68152-formula148"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x108.png"  xlink:type="simple"/></disp-formula><p>Hence, substituting the above values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x109.png" xlink:type="simple"/></inline-formula> in (7), we obtain</p><disp-formula id="scirp.68152-formula149"><label>(36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x110.png"  xlink:type="simple"/></disp-formula><p>Using boundary condition at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x111.png" xlink:type="simple"/></inline-formula> on equation (36) we obtain the values of a, b, c, d and e, as</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x112.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x113.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x114.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x115.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x112.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x113.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x114.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x115.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x116.png" xlink:type="simple"/></inline-formula></p><p>Thus, the final approximation solution of the BVP (33) can be written as</p><disp-formula id="scirp.68152-formula150"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x117.png"  xlink:type="simple"/></disp-formula><p>The comparison of the approximate solution of Example 2 obtained with the help of PSAM and the approximate solution using HPM [<xref ref-type="bibr" rid="scirp.68152-ref2">2</xref>] is given in <xref ref-type="table" rid="table2">Table 2</xref>. From the numerical results, it is clear that the PSAM is more efficient and accurate. By increasing the order of approximation more accuracy can be obtained.</p><p>Example 3</p><p>Consider the following twelve-order problem</p><disp-formula id="scirp.68152-formula151"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x118.png"  xlink:type="simple"/></disp-formula><p>with the following boundary conditions</p><disp-formula id="scirp.68152-formula152"><label>(38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x119.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68152-formula153"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x120.png"  xlink:type="simple"/></disp-formula><p>The exact solution is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x121.png" xlink:type="simple"/></inline-formula>.</p><p>The given 12th order BVP (37) is transformed to systems of ODEs such that we have</p><disp-formula id="scirp.68152-formula154"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x122.png"  xlink:type="simple"/></disp-formula><p>with the boundary conditions (at<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x123.png" xlink:type="simple"/></inline-formula>)</p><disp-formula id="scirp.68152-formula155"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x124.png"  xlink:type="simple"/></disp-formula><p>Since, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x125.png" xlink:type="simple"/></inline-formula>, we have Equation (14) as</p><disp-formula id="scirp.68152-formula156"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x126.png"  xlink:type="simple"/></disp-formula><p>Hence for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x127.png" xlink:type="simple"/></inline-formula> we obtain the following</p><disp-formula id="scirp.68152-formula157"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x128.png"  xlink:type="simple"/></disp-formula><p>Hence, substituting the above values of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x129.png" xlink:type="simple"/></inline-formula> in (7), we obtain</p><disp-formula id="scirp.68152-formula158"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/2-7403185x130.png"  xlink:type="simple"/></disp-formula><p>Using boundary condition at <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x131.png" xlink:type="simple"/></inline-formula> in Equation (40) we obtain the values of a, b, c, d, e and f, as</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x132.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x133.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x134.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x135.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x136.png" xlink:type="simple"/></inline-formula>and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x132.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x133.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x134.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x135.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x136.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/2-7403185x137.png" xlink:type="simple"/></inline-formula>.</p><p>Thus, substituting the values a, b, c, d, e and f in (40), the final approximation solution of BVP (37) can be written as</p><disp-formula id="scirp.68152-formula159"><graphic  xlink:href="http://html.scirp.org/file/2-7403185x138.png"  xlink:type="simple"/></disp-formula><p>The comparison of the approximate solution of Example 3 obtained with the help of PSAM and the approximate solution using HPM [<xref ref-type="bibr" rid="scirp.68152-ref2">2</xref>] is given in <xref ref-type="table" rid="table3">Table 3</xref>. From the numerical results, it is clear that the PSAM is more efficient and accurate. By increasing the order of approximation more accuracy can be obtained.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, the Power Series Approximation Method has been applied to obtain the numerical solution of linear and nonlinear generalized N<sup>th</sup> order boundary value problems. The PSAM requires no discretization, linea-rization or perturbation. By increasing the order of approximation more accuracy can be obtained. Comparison of the results obtained with existing techniques [<xref ref-type="bibr" rid="scirp.68152-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.68152-ref2">2</xref>] shows that the PSAM is more efficient and accurate. Hence, it is easier and more economical to apply PSAM in solving BVPs.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Comparison of results of PSAM with Variational Iteration Method (VIM)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >X</th><th align="center" valign="middle" >Exact Solution</th><th align="center" valign="middle" >PSAM</th><th align="center" valign="middle" >VIM</th></tr></thead><tr><td align="center" valign="middle" >0.00</td><td align="center" valign="middle" >1.0000000</td><td align="center" valign="middle" >1.0000000</td><td align="center" valign="middle" >1.000000</td></tr><tr><td align="center" valign="middle" >0.10</td><td align="center" valign="middle" >1.0948376</td><td align="center" valign="middle" >1.0948376</td><td align="center" valign="middle" >0.994054</td></tr><tr><td align="center" valign="middle" >0.20</td><td align="center" valign="middle" >1.1787359</td><td align="center" valign="middle" >1.1787359</td><td align="center" valign="middle" >0.931864</td></tr><tr><td align="center" valign="middle" >0.30</td><td align="center" valign="middle" >1.2508567</td><td align="center" valign="middle" >1.2508568</td><td align="center" valign="middle" >0.769356</td></tr><tr><td align="center" valign="middle" >0.40</td><td align="center" valign="middle" >1.3104793</td><td align="center" valign="middle" >1.3104800</td><td align="center" valign="middle" >0.784691</td></tr><tr><td align="center" valign="middle" >0.50</td><td align="center" valign="middle" >1.3570081</td><td align="center" valign="middle" >1.3570112</td><td align="center" valign="middle" >0.659287</td></tr><tr><td align="center" valign="middle" >0.60</td><td align="center" valign="middle" >1.3899781</td><td align="center" valign="middle" >1.3899892</td><td align="center" valign="middle" >0.537115</td></tr><tr><td align="center" valign="middle" >0.70</td><td align="center" valign="middle" >1.4090599</td><td align="center" valign="middle" >1.4090924</td><td align="center" valign="middle" >0.381117</td></tr><tr><td align="center" valign="middle" >0.80</td><td align="center" valign="middle" >1.4140628</td><td align="center" valign="middle" >1.4141457</td><td align="center" valign="middle" >0.240714</td></tr><tr><td align="center" valign="middle" >0.90</td><td align="center" valign="middle" >1.4049369</td><td align="center" valign="middle" >1.4051257</td><td align="center" valign="middle" >0.129106</td></tr><tr><td align="center" valign="middle" >1.00</td><td align="center" valign="middle" >1.3817733</td><td align="center" valign="middle" >1.3821676</td><td align="center" valign="middle" >0.000000</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Comparison of results of PSAM with HPM</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >X</th><th align="center" valign="middle" >Exact Solution</th><th align="center" valign="middle" >PSAM</th><th align="center" valign="middle" >HPM</th></tr></thead><tr><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >0.100000000</td><td align="center" valign="middle" >0.100000000</td><td align="center" valign="middle" >0.1000000000</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >0.122140276</td><td align="center" valign="middle" >0.122140276</td><td align="center" valign="middle" >0.1221408246</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >0.149182470</td><td align="center" valign="middle" >0.149182470</td><td align="center" valign="middle" >0.1491833581</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >0.182211880</td><td align="center" valign="middle" >0.182211878</td><td align="center" valign="middle" >0.1822127686</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >0.222554093</td><td align="center" valign="middle" >0.222554055</td><td align="center" valign="middle" >0.2225546413</td></tr><tr><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >0.271828183</td><td align="center" valign="middle" >0.271827885</td><td align="center" valign="middle" >0.2718281799</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Comparison of results of PSAM with HPM</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >X</th><th align="center" valign="middle" >Exact Solution</th><th align="center" valign="middle" >PSAM</th><th align="center" valign="middle" >HPM</th></tr></thead><tr><td align="center" valign="middle" >0.0</td><td align="center" valign="middle" >10.000000000</td><td align="center" valign="middle" >10.000000000</td><td align="center" valign="middle" >10.000000000</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >8.187307531</td><td align="center" valign="middle" >8.187318703</td><td align="center" valign="middle" >8.187308703</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >6.703200460</td><td align="center" valign="middle" >6.703218540</td><td align="center" valign="middle" >6.703208540</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >5.488116361</td><td align="center" valign="middle" >5.488134449</td><td align="center" valign="middle" >5.488114451</td></tr><tr><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >4.493289641</td><td align="center" valign="middle" >4.493300834</td><td align="center" valign="middle" >4.493289646</td></tr><tr><td align="center" valign="middle" >1.0</td><td align="center" valign="middle" >3.678794412</td><td align="center" valign="middle" >3.678794408</td><td align="center" valign="middle" >3.678794453</td></tr></tbody></table></table-wrap></sec><sec id="s6"><title>Cite this paper</title><p>Ignatius N. 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