<?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.2013.32018</article-id><article-id pub-id-type="publisher-id">AJCM-33539</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>
 
 
  New Improved Variational Homotopy Perturbation Method for Bratu-Type Problems
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>lusola</surname><given-names>Ezekiel Abolarin</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 Industrial Mathematics, Landmark University, Omu Aran, Nigeria</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>sola4one@yahoo.com</email></corresp></author-notes><pub-date pub-type="epub"><day>17</day><month>06</month><year>2013</year></pub-date><volume>03</volume><issue>02</issue><fpage>110</fpage><lpage>113</lpage><history><date date-type="received"><day>January</day>	<month>31,</month>	<year>2013</year></date><date date-type="rev-recd"><day>March</day>	<month>1,</month>	<year>2013</year>	</date><date date-type="accepted"><day>March</day>	<month>29,</month>	<year>2013</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>
 
 
   This research paper deals with the boundary and initial value problems for the Bratu-type model by using the New Improved Variational Homotopy Perturbation Method. The New Method does not require discritization, linearization or any restrictive assumption of any form in providing analytical or approximate solutions to linear and nonlinear equation without the integral related with nonlinear term. Theses virtues make it to be reliable and its efficiency is demonstrated with numerical examples. 
 
</p></abstract><kwd-group><kwd>Bratu-Type Problem; Variational Iteration Method; Homotopy Perturbation Method; New Improved Variational Homotopy Perturbation Method; Boundary Value Problems; Initial Value Problems</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The Bratu-type boundary value problem in one-dimensional planar coordinates</p><disp-formula id="scirp.33539-formula89809"><label>(1.1)</label><graphic position="anchor" xlink:href="4-1100090\bac460c9-eec5-48cb-8e43-75745d07e578.jpg"  xlink:type="simple"/></disp-formula><p>arises from a simplification of the solid fuel ignition model in thermal combustion theory, physical applications ranging from chemical reaction theory, radiative heat transfer and nanotechnology to the expansion of universe [1-5]. The initial value problem of the Bratutype model [<xref ref-type="bibr" rid="scirp.33539-ref5">5</xref>] is given by</p><disp-formula id="scirp.33539-formula89810"><label>(1.2)</label><graphic position="anchor" xlink:href="4-1100090\da51beb3-5b0b-4116-aaea-88d96846ff9b.jpg"  xlink:type="simple"/></disp-formula><p>Due to its mathematical and physical properties, the Bratu-type problems have been studied extensively [4-8]. Recently, Wazwaz [<xref ref-type="bibr" rid="scirp.33539-ref5">5</xref>] applied Adomian decomposition method to study the Bratu-type equations, Syam [<xref ref-type="bibr" rid="scirp.33539-ref4">4</xref>] discussed the Bratu-type problems with variational iteration method, and Feng [<xref ref-type="bibr" rid="scirp.33539-ref6">6</xref>] considered these problems by means of modified homotopy perturbation method. However, the existing methods such as Adomian decomposition method, variational iteration method and homotopy perturbation method involve the computation of Adomian polynomials, and the integral related with e<sup>u</sup> or the perturbation of small parameters, this leads to increase the numerical computation cost and narrow down their applications. To avoid these disadvantages, Lin Jin [<xref ref-type="bibr" rid="scirp.33539-ref9">9</xref>] proposed a modified variational iteration method to solve the Bratu problems, based upon the Taylor series expansion. In order to improve on what Lin Jin [<xref ref-type="bibr" rid="scirp.33539-ref9">9</xref>] has done, we introduce the New Improved Variational Homotopy Perturbation Method for Bratu-Type Problems which is a time cost effective and uses friendly.</p></sec><sec id="s2"><title>2. Variational Iteration Method and Its Modification</title><p>To illustrate the basic concepts of the variational iteration method [10-12], we consider the following differential equation:</p><disp-formula id="scirp.33539-formula89811"><label>(2.1)</label><graphic position="anchor" xlink:href="4-1100090\0bf7e39e-6be5-4716-b737-45eee0837ddb.jpg"  xlink:type="simple"/></disp-formula><p>where L is a linear operator, N is a nonlinear operator, and <img src="4-1100090\b2432c52-3f2b-4747-96c0-7be099490096.jpg" /> is an inhomogeneous term. Then, we can construct a correct functional as follows:</p><disp-formula id="scirp.33539-formula89812"><label>(2.2)</label><graphic position="anchor" xlink:href="4-1100090\8d825978-8ceb-4d3a-8c22-058fc8cae1bd.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-1100090\1b3d39fc-23e3-4f6e-9b39-fa339cd54a25.jpg" /> is a general Lagrange multiplier [10,11], which can be optimally identified via variational theory. The second term on the right is called the correction and <img src="4-1100090\4a201d0b-74c5-481c-ba74-6bf796ab7393.jpg" /> is considered as a restricted variation, i.e.<img src="4-1100090\20b8179d-2cef-4659-a353-06a6fd6b1c20.jpg" />. For the nonlinear differential Equation (2.1), the nonlinear term <img src="4-1100090\93485d0c-24a3-451b-8274-7dbcd7146653.jpg" /> can be expressed in Taylor series</p><p><img src="4-1100090\c478eb3f-2bc2-4809-bdbc-9b78abc68a1b.jpg" /></p><p>We determine the Lagrange multiplier <img src="4-1100090\d21da0d5-7d20-4971-8d37-01ebd51ee248.jpg" /> in the correction functional (2.2) with the series above. This results in the following iteration formula:</p><disp-formula id="scirp.33539-formula89813"><label>(2.3)</label><graphic position="anchor" xlink:href="4-1100090\e4c9a6cb-9779-4dd8-941e-3d77d7311c49.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. New Imprved Variational Homotopy Perturbation Method</title><p>To illustrate the basic concept of the New Improved Variational Homotopy Perturbation Method, we consider the following general differential equation:</p><disp-formula id="scirp.33539-formula89814"><label>(3.1)</label><graphic position="anchor" xlink:href="4-1100090\28c186b7-c743-46e4-8bfd-ffb1949032fb.jpg"  xlink:type="simple"/></disp-formula><p>where L is a linear operator, N a non-linear operator, and <img src="4-1100090\eb935e34-01ed-480c-8368-d74ba063eb6a.jpg" /> is the homogenous term. By the variational iteration method, we construct a correction functional :</p><disp-formula id="scirp.33539-formula89815"><label>(3.2)</label><graphic position="anchor" xlink:href="4-1100090\332bee94-ac00-495a-b63c-dbf0cf85a0d5.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-1100090\10fbdebd-d759-443a-9c8f-8390f8a64ca8.jpg" /></p><p>Hence,</p><disp-formula id="scirp.33539-formula89816"><label>(3.3)</label><graphic position="anchor" xlink:href="4-1100090\499ebea5-a81e-4bdd-93d4-405c231d5da5.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="4-1100090\9b8eee1c-c0d4-4ddd-8f52-f393de13a56f.jpg" /> is a Lagrange multiplier according to Barari et al. [<xref ref-type="bibr" rid="scirp.33539-ref1">1</xref>], which can be identified optimally via variational theory. The subscript n denotes the n-th approximation, <img src="4-1100090\60885327-ad4b-4163-85e7-416660bd8168.jpg" />is considered as a restricted variational, that is,<img src="4-1100090\032e58c7-cad5-44e4-8fb5-c304e6a57e14.jpg" />; and Equation (3.2) is called a correction functional.</p><p>Now we implement the New Improved Variational Homotopy Perturbation Method to the correction functional in Equation (3.3). we have the following:</p><disp-formula id="scirp.33539-formula89817"><label>(3.4)</label><graphic position="anchor" xlink:href="4-1100090\da184ad1-e081-4d1c-92f7-0a4b6081e2c0.jpg"  xlink:type="simple"/></disp-formula><p>This can be expressed as:</p><disp-formula id="scirp.33539-formula89818"><label>(3.5)</label><graphic position="anchor" xlink:href="4-1100090\9c5ff50c-af74-4be8-8af2-d81af3a459ca.jpg"  xlink:type="simple"/></disp-formula><p>Hence, Equation (3.5) represents the coupling of variational iteration and Homotopy Perturbation methods.</p><p>The comparison of the coefficients of like powers of P gives solutions of various orders, this implies:</p><disp-formula id="scirp.33539-formula89819"><label>(3.6)</label><graphic position="anchor" xlink:href="4-1100090\3abedf96-3d13-4a39-b735-e18623489fd0.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s4"><title>4. Numerical Examples</title><p>In this section, we will apply the New Improved Variational Homotopy Perturbation Method for soving boundary value problems or Initial value problems of the Bratu-type equation. Numerical results are shown to illustrate the efficiency of the method.</p><p>Example 1: We consider the Bratu-type equation [<xref ref-type="bibr" rid="scirp.33539-ref12">12</xref>]</p><disp-formula id="scirp.33539-formula89820"><label>(4.1)</label><graphic position="anchor" xlink:href="4-1100090\d900c8a3-af3a-4621-91d9-5e9716f042d5.jpg"  xlink:type="simple"/></disp-formula><p>with the boundary conditions</p><p><img src="4-1100090\ffbd41bd-2fe8-4ca9-990b-34f5b084e7b4.jpg" /></p><p>Based on the Taylor series of<img src="4-1100090\7fbf2635-8668-46c7-a1de-562fba6f8caa.jpg" />,</p><disp-formula id="scirp.33539-formula89821"><label>(4.2)</label><graphic position="anchor" xlink:href="4-1100090\55f60551-ff45-4da2-8dfd-ba563b279b81.jpg"  xlink:type="simple"/></disp-formula><p>Correction functional is given is given as</p><disp-formula id="scirp.33539-formula89822"><label>(4.3)</label><graphic position="anchor" xlink:href="4-1100090\324faf01-9a58-4c26-8f64-4c39d1ab08bd.jpg"  xlink:type="simple"/></disp-formula><p>the NIVHPM is given as</p><disp-formula id="scirp.33539-formula89823"><label>(4.4)</label><graphic position="anchor" xlink:href="4-1100090\51f65554-4e1d-420b-98c7-a04c08305faa.jpg"  xlink:type="simple"/></disp-formula><p>Comparing the coefficients of like powers of p, we have:</p><p><img src="4-1100090\7943d1bc-6032-4fb2-90dd-b0b30683a7ff.jpg" /></p><p>Example 2: We next consider the Bratu-type equation [<xref ref-type="bibr" rid="scirp.33539-ref12">12</xref>]</p><disp-formula id="scirp.33539-formula89824"><label>(4.5)</label><graphic position="anchor" xlink:href="4-1100090\c614f37e-c8de-4db4-859e-c8ecbea1b9ef.jpg"  xlink:type="simple"/></disp-formula><p>with the boundary conditions</p><p><img src="4-1100090\c137a421-a7b4-4ad8-89d2-92cd3cdd39ea.jpg" /></p><p>Using the Taylor series of<img src="4-1100090\0350fbc0-0eb9-4757-9d43-292badacad4a.jpg" />, the correction functional is given as</p><disp-formula id="scirp.33539-formula89825"><label>(4.6)</label><graphic position="anchor" xlink:href="4-1100090\350e76df-0521-49d9-8525-545fc57b83e7.jpg"  xlink:type="simple"/></disp-formula><p>the NIVHPM is given as</p><disp-formula id="scirp.33539-formula89826"><label>(4.7)</label><graphic position="anchor" xlink:href="4-1100090\f998abd7-71cc-44af-9dac-3fd7d7fa5ff1.jpg"  xlink:type="simple"/></disp-formula><p>Comparing the coefficients of like powers of p, we have:</p><p><img src="4-1100090\ac691cf1-6ab5-49c2-9124-b83ceb46cb24.jpg" /></p><p>Example 3: We again consider the Bratu-type equation [<xref ref-type="bibr" rid="scirp.33539-ref9">9</xref>]</p><disp-formula id="scirp.33539-formula89827"><label>(4.8)</label><graphic position="anchor" xlink:href="4-1100090\4ebba2b2-138a-4b81-a9a3-5822ad02b209.jpg"  xlink:type="simple"/></disp-formula><p>with the boundary conditions</p><p><img src="4-1100090\4f7ab98c-31d0-4732-97bd-0feb96fdbd6a.jpg" /></p><p>Using the Taylor series of<img src="4-1100090\e0bdd2dc-e4fe-4882-a34c-adcf5c1d4652.jpg" />, the correction functional is given as</p><disp-formula id="scirp.33539-formula89828"><label>(4.9)</label><graphic position="anchor" xlink:href="4-1100090\5a4a5893-b47f-479e-ae1a-00f39a925f02.jpg"  xlink:type="simple"/></disp-formula><p>the NIVHPM is given as</p><disp-formula id="scirp.33539-formula89829"><label>(4.10)</label><graphic position="anchor" xlink:href="4-1100090\684e31ee-b414-4ace-8617-0a9cdd0e72ce.jpg"  xlink:type="simple"/></disp-formula><p>Comparing the coefficients of like powers of p, we have:</p><disp-formula id="scirp.33539-formula89830"><label>(4.11)</label><graphic position="anchor" xlink:href="4-1100090\39aada85-40f3-4061-9224-28319870388a.jpg"  xlink:type="simple"/></disp-formula></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, New Improved Variational Homotopy Perturbation Method has been successfully applied to find the solution of Bratu-type problem and the results obtained were compared favourably with the two convectional variational iteration and Homotopy Perturbation Method. It can be concluded that the NIVHPM is a very powerful and efficient technique for finding approximate solutions for wide classes of problems. It is worth mentioning that the Method is the computational cost friendly.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.33539-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">J. P. Boyd, “An Analytical and Numerical Study of the Two-Dimentional Bratu Equation,” Journal of Scientific Computing, Vol. 1, No. 2, 1986, pp. 183-206. 
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