<?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">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2016.411203</article-id><article-id pub-id-type="publisher-id">JAMP-72119</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>
 
 
  Gauss-Legendre Iterative Methods and Their Applications on Nonlinear Systems and BVP-ODEs
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhongli</surname><given-names>Liu</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>Guoqing</surname><given-names>Sun</given-names></name><xref ref-type="aff" rid="aff2"><sup>2</sup></xref></contrib></contrib-group><aff id="aff2"><addr-line>College of Renai, Tianjin University, Tianjin, China</addr-line></aff><aff id="aff1"><addr-line>College of Biochemical Engineering, Beijing Union University, Beijing, China</addr-line></aff><pub-date pub-type="epub"><day>10</day><month>11</month><year>2016</year></pub-date><volume>04</volume><issue>11</issue><fpage>2038</fpage><lpage>2046</lpage><history><date date-type="received"><day>October</day>	<month>24,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>November</month>	<year>15,</year>	</date><date date-type="accepted"><day>November</day>	<month>18,</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 group of Gauss-Legendre iterative methods with cubic convergence for solving nonlinear systems are proposed. We construct the iterative schemes based on Gauss-Legendre quadrature formula. The cubic convergence and error equation are proved theoretically, and demonstrated numerically. Several numerical examples for solving the system of nonlinear equations and boundary-value problems of nonlinear ordinary differential equations (ODEs) are provided to illustrate the efficiency and performance of the suggested iterative methods.
 
</p></abstract><kwd-group><kwd>Iterative Method</kwd><kwd> Gauss-Legendre Quadrature Formula</kwd><kwd> Nonlinear Systems</kwd><kwd> Third-Order Convergence</kwd><kwd> Nonlinear ODEs</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We consider the general form of a system of nonlinear equations as follows:</p><disp-formula id="scirp.72119-formula85"><label>, (1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x2.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x3.png" xlink:type="simple"/></inline-formula> is a given nonlinear vector function, and each function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x4.png" xlink:type="simple"/></inline-formula> can be thought of as mapping of a vector<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x5.png" xlink:type="simple"/></inline-formula>, which is the n- dimensional space <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x6.png" xlink:type="simple"/></inline-formula> into the real number R.</p><p>Numerical solutions for systems of nonlinear equations have always appealed greatly to people in scientific computation and engineering fields. Some boundary-value problems of nonlinear ordinary differential equations (ODEs) can be transformed to nonlinear systems like (1) by the finite difference method. Constructing an efficiently iterative method to approximate the root <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x7.png" xlink:type="simple"/></inline-formula> (such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x8.png" xlink:type="simple"/></inline-formula>) of Equation (1) is a typical and important issue in nonlinear numerical computation. The Newton’s method (see [<xref ref-type="bibr" rid="scirp.72119-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.72119-ref2">2</xref>] ) is one of the widely used methods for solving nonlinear equations by iteration as follows:</p><disp-formula id="scirp.72119-formula86"><label>, (2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x9.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x10.png" xlink:type="simple"/></inline-formula> is the inverse of first Fr&#233;chet derivative <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x11.png" xlink:type="simple"/></inline-formula> which is a Jacobian matrix of the nonlinear vector function<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x12.png" xlink:type="simple"/></inline-formula>. It converges quadratically when an initial guess value <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x13.png" xlink:type="simple"/></inline-formula> is close to the root <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x14.png" xlink:type="simple"/></inline-formula> of Equation (1). In recent years, several iterative methods have been used to solve nonlinear equations and systems of nonlinear equations. In order to improve the order of convergence, a few two-step variants of Newton’s methods with cubic convergence have been proposed in some literature [<xref ref-type="bibr" rid="scirp.72119-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.72119-ref11">11</xref>] and references therein for solving systems of nonlinear equations. S. We era-</p><p>koon and T. Fernando [<xref ref-type="bibr" rid="scirp.72119-ref5">5</xref>] using the Newton theorem<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x15.png" xlink:type="simple"/></inline-formula>,</p><p>proposed the Newton-type method with third-order convergence for nonlinear equation and systems. M. Darvishi and A. Barati [<xref ref-type="bibr" rid="scirp.72119-ref6">6</xref>] received a third-order convergence iterative method based on Adomian decomposition method to the systems of nonlinear equations. M. Frontini and E. Sormani [<xref ref-type="bibr" rid="scirp.72119-ref7">7</xref>] presented third-order midpoint-methods using numerical quadrature formula. A. Cordero and J. R. Torregrsa [<xref ref-type="bibr" rid="scirp.72119-ref8">8</xref>] developed third-order convergence Newton-Simpson’s method and Open Newton’s method using the simple Simpson’s rule and an open quadrature formula of high order respectively. These are all classic two-step Newton-type methods to approximate the root of a system of nonlinear equations.</p><p>In Section 2 of this paper, we propose a group of two-step iterative methods with third-order convergence by Gauss-Legendre quadrature formula [<xref ref-type="bibr" rid="scirp.72119-ref12">12</xref>] :</p><disp-formula id="scirp.72119-formula87"><label>, (3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x16.png"  xlink:type="simple"/></disp-formula><p>where the necessary symmetrical conditions is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x17.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x18.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x19.png" xlink:type="simple"/></inline-formula>. (4)</p><p>Several numerical examples are provided in Section 3 using Gauss-Legendre iterative method for solving systems of nonlinear equations and boundary-value problems of nonlinear ODEs, and we finally make conclusions in Section 4.</p></sec><sec id="s2"><title>2. The Iterative Methods and Cubic Convergence</title><p>Assume <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x20.png" xlink:type="simple"/></inline-formula> be a Fr&#233;chet differentiable function in a convex<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x21.png" xlink:type="simple"/></inline-formula>. We have the mean-value theorem of multivariable vectors function F(x) in [<xref ref-type="bibr" rid="scirp.72119-ref1">1</xref>] :</p><disp-formula id="scirp.72119-formula88"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x22.png"  xlink:type="simple"/></disp-formula><p>Using the left rectangular integral rule:</p><disp-formula id="scirp.72119-formula89"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x23.png"  xlink:type="simple"/></disp-formula><p>And by<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x24.png" xlink:type="simple"/></inline-formula>, we can get Newton’s Method (2).</p><p>Now, we apply the Gauss-Legendre quadrature formula (3) to approximate the integral on the right side of Equation (5), that is,</p><disp-formula id="scirp.72119-formula90"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x25.png"  xlink:type="simple"/></disp-formula><p>and using <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x26.png" xlink:type="simple"/></inline-formula> we have</p><disp-formula id="scirp.72119-formula91"><label>. (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x27.png"  xlink:type="simple"/></disp-formula><p>Herein, taking x as the next iterative step of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x28.png" xlink:type="simple"/></inline-formula>, we get the following implicit structure:</p><disp-formula id="scirp.72119-formula92"><label>. (9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x29.png"  xlink:type="simple"/></disp-formula><p>We use the k-th iteration <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x30.png" xlink:type="simple"/></inline-formula> of the Newton’s method to replace <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x31.png" xlink:type="simple"/></inline-formula> on the right side of the expression (9), and we construct the following group of two-step iterative schemes:</p><disp-formula id="scirp.72119-formula93"><label>. (10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x32.png"  xlink:type="simple"/></disp-formula><p>We state and prove the convergence theorem for the schemes (10) as follows:</p><p>Theorem Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x33.png" xlink:type="simple"/></inline-formula> be a k-time Fr&#233;chet differentiable function in a convex set D with a root <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x34.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x35.png" xlink:type="simple"/></inline-formula> be close to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x36.png" xlink:type="simple"/></inline-formula>, then the group of iterative methods (10) is cubically convergent, and the error equation is</p><disp-formula id="scirp.72119-formula94"><label>. (11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x37.png"  xlink:type="simple"/></disp-formula><p>Proof. As<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x38.png" xlink:type="simple"/></inline-formula>, and noting that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x39.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x38.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x39.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x40.png" xlink:type="simple"/></inline-formula>.</p><p>By Taylor’s expansion, we have</p><disp-formula id="scirp.72119-formula95"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x41.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.72119-formula96"><label>. (13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x42.png"  xlink:type="simple"/></disp-formula><p>Then, suppose that</p><disp-formula id="scirp.72119-formula97"><label>, (14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x43.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.72119-formula98"><label>. (15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x44.png"  xlink:type="simple"/></disp-formula><p>The inverse of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x45.png" xlink:type="simple"/></inline-formula> is given by</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x46.png" xlink:type="simple"/></inline-formula>,</p><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x47.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x48.png" xlink:type="simple"/></inline-formula> will be satisfied the definition of the following inversion.</p><disp-formula id="scirp.72119-formula99"><label>. (16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x49.png"  xlink:type="simple"/></disp-formula><p>That is</p><disp-formula id="scirp.72119-formula100"><label>. (17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x50.png"  xlink:type="simple"/></disp-formula><p>From (17), we have</p><disp-formula id="scirp.72119-formula101"><label>. (18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x51.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.72119-formula102"><label>. (19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x52.png"  xlink:type="simple"/></disp-formula><p>And</p><disp-formula id="scirp.72119-formula103"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x53.png"  xlink:type="simple"/></disp-formula><p>By the first step of (10), we have</p><disp-formula id="scirp.72119-formula104"><label>, (21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x54.png"  xlink:type="simple"/></disp-formula><p>Here, suppose<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x55.png" xlink:type="simple"/></inline-formula>.</p><p>So,</p><disp-formula id="scirp.72119-formula105"><label>, (22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x56.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.72119-formula106"><label>. (23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x57.png"  xlink:type="simple"/></disp-formula><p>Furthermore,</p><disp-formula id="scirp.72119-formula107"><label>, (24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x58.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.72119-formula108"><label>. (25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x59.png"  xlink:type="simple"/></disp-formula><p>Then,</p><disp-formula id="scirp.72119-formula109"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x60.png"  xlink:type="simple"/></disp-formula><p>Let</p><disp-formula id="scirp.72119-formula110"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x61.png"  xlink:type="simple"/></disp-formula><p>By the conditions (4), we have</p><disp-formula id="scirp.72119-formula111"><label>. (28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x62.png"  xlink:type="simple"/></disp-formula><p>So the iterative schemes (10) can be written as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x63.png" xlink:type="simple"/></inline-formula>. Subtracting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x63.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x64.png" xlink:type="simple"/></inline-formula> from both sides of this equation, we can obtain</p><disp-formula id="scirp.72119-formula112"><label>, (29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x65.png"  xlink:type="simple"/></disp-formula><p>that is</p><disp-formula id="scirp.72119-formula113"><label>(30)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x66.png"  xlink:type="simple"/></disp-formula><p>Therefore, the error equation is</p><disp-formula id="scirp.72119-formula114"><label>. (31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x67.png"  xlink:type="simple"/></disp-formula><p>This shows that the group of iterative methods (10) is third-order convergent.</p><p>As for the iterative methods (10), when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x68.png" xlink:type="simple"/></inline-formula>, then it can be transformed to the following form:</p><disp-formula id="scirp.72119-formula115"><label>. (32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x69.png"  xlink:type="simple"/></disp-formula><p>When<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x70.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x71.png" xlink:type="simple"/></inline-formula>is a parameter, then the methods (10) can be written as follows:</p><disp-formula id="scirp.72119-formula116"><label>. (33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x72.png"  xlink:type="simple"/></disp-formula><p>Especially, we take the parameter <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x73.png" xlink:type="simple"/></inline-formula> in the iterative method (33) to make applications in the following section.</p></sec><sec id="s3"><title>3. Numerical Examples</title><p>The iterative method (33) with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x74.png" xlink:type="simple"/></inline-formula> is demonstrated for solving systems of nonlinear equations and some two-point boundary-value problems of nonlinear ODEs.</p><p>Example 1. Consider a system of nonlinear equations with variables<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x75.png" xlink:type="simple"/></inline-formula>:</p><disp-formula id="scirp.72119-formula117"><label>, (34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x76.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x77.png" xlink:type="simple"/></inline-formula> is the guess value. We can get the exact solution <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x77.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x78.png" xlink:type="simple"/></inline-formula> by the iterative method (33) for Equation (34). The numerical results are shown in <xref ref-type="table" rid="table1">Table 1</xref>, in which k refers to the number of iterations.</p><p>Example 2. Consider solving the following two-point boundary-value problem of nonlinear ODE:</p><disp-formula id="scirp.72119-formula118"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x79.png"  xlink:type="simple"/></disp-formula><p>We discretize the nonlinear ODE (35) with the finite difference method. Taking nodes<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x80.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x81.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x81.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x82.png" xlink:type="simple"/></inline-formula> herein, we can obtain the following system of nine-variables nonlinear equations:</p><disp-formula id="scirp.72119-formula119"><label>, (36)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x83.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x84.png" xlink:type="simple"/></inline-formula>. Using the iterative method (33), we get the numerical solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x84.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x85.png" xlink:type="simple"/></inline-formula> of Equation (36), that is,</p><disp-formula id="scirp.72119-formula120"><graphic  xlink:href="http://html.scirp.org/file/6-1720726x86.png"  xlink:type="simple"/></disp-formula><p>The numerical results for the system of nonlinear Equations (36) derived from ODE (35) are shown in <xref ref-type="table" rid="table2">Table 2</xref>.</p><p>According to results of the above two numerical experiments, the iterative method (33) can achieve third-order convergence for systems of nonlinear equations, and their numerical solutions show also the method is feasible.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The numerical solutions and errors of the system of Equation (34) using the method (33)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x87.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >2</th><th align="center" valign="middle" >3</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >5</th><th align="center" valign="middle" >6</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x88.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.1943e−1</td><td align="center" valign="middle" >4.3758e−3</td><td align="center" valign="middle" >1.6660e−8</td><td align="center" valign="middle" >9.2481e−25</td><td align="center" valign="middle" >1.5819e−73</td><td align="center" valign="middle" >7.9180e−220</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x89.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.4602e−0</td><td align="center" valign="middle" >1.7537e−2</td><td align="center" valign="middle" >6.6640e−8</td><td align="center" valign="middle" >3.6992e−24</td><td align="center" valign="middle" >6.3278e−73</td><td align="center" valign="middle" >3.1672e−219</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The numerical solutions and errors of the system of nonlinear Equation (36)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x90.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >2</th><th align="center" valign="middle" >3</th><th align="center" valign="middle" >4</th></tr></thead><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x91.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >4.9234e−4</td><td align="center" valign="middle" >5.63305e−14</td><td align="center" valign="middle" >8.6475e−17</td><td align="center" valign="middle" >8.6475e−17</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x92.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.3365e−4</td><td align="center" valign="middle" >9.35871e−15</td><td align="center" valign="middle" >9.7017e−45</td><td align="center" valign="middle" >1.5685e−134</td></tr></tbody></table></table-wrap><p>Example 3. Solving the following two-point nonlinear boundary-value problem of ODE with exact solution:</p><disp-formula id="scirp.72119-formula121"><label>. (37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x93.png"  xlink:type="simple"/></disp-formula><p>The exact solution for this problem of ODE (37) is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x94.png" xlink:type="simple"/></inline-formula>. We now</p><p>find the numerical solutions using the present method and compare them with the exact solution<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x95.png" xlink:type="simple"/></inline-formula>.</p><p>By the finite difference method, partitioning the interval<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x96.png" xlink:type="simple"/></inline-formula>:<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x97.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x96.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x97.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x98.png" xlink:type="simple"/></inline-formula>.</p><p>Let<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x99.png" xlink:type="simple"/></inline-formula>, and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x99.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x100.png" xlink:type="simple"/></inline-formula>. And</p><p>using the numerical differential formula for the second derivative<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x101.png" xlink:type="simple"/></inline-formula>, and the first derivative<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x102.png" xlink:type="simple"/></inline-formula>, we take <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x101.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x102.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x103.png" xlink:type="simple"/></inline-formula> herein, and</p><p>hence obtain the following system of nonlinear equations with nine variables:</p><disp-formula id="scirp.72119-formula122"><label>, (38)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/6-1720726x104.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x105.png" xlink:type="simple"/></inline-formula> is an initial value. We obtain the approximate numerical solutions of this problem with the method (33) (iteration number k = 5):</p><disp-formula id="scirp.72119-formula123"><graphic  xlink:href="http://html.scirp.org/file/6-1720726x106.png"  xlink:type="simple"/></disp-formula><p>Comparison of the numerical results of the boundary-value problem of ODE (37) and the exact solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x107.png" xlink:type="simple"/></inline-formula> are shown in <xref ref-type="table" rid="table3">Table 3</xref>, in which <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x107.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x108.png" xlink:type="simple"/></inline-formula> refers to the nodes.</p><p>The error comparisons of the numerical solutions and exact solutions at different nodes <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x109.png" xlink:type="simple"/></inline-formula> for solving the problem of ODE (37) are shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>.</p><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title>Numerical comparison results for the problem of ODE (37)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x110.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Numerical solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x111.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >Exact solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x112.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" >The errors <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/6-1720726x113.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >0.1</td><td align="center" valign="middle" >1.00412287612219…</td><td align="center" valign="middle" >1.0050041680558035039…</td><td align="center" valign="middle" >8.812e−04</td></tr><tr><td align="center" valign="middle" >0.2</td><td align="center" valign="middle" >1.01834640006185…</td><td align="center" valign="middle" >1.0200667556190758933…</td><td align="center" valign="middle" >1.720e−03</td></tr><tr><td align="center" valign="middle" >0.3</td><td align="center" valign="middle" >1.04286614560037…</td><td align="center" valign="middle" >1.0453385141288604742…</td><td align="center" valign="middle" >2.472e−03</td></tr><tr><td align="center" valign="middle" >0.4</td><td align="center" valign="middle" >1.07798462092560…</td><td align="center" valign="middle" >1.0810723718384549485…</td><td align="center" valign="middle" >3.087e−03</td></tr><tr><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >1.12411585747856…</td><td align="center" valign="middle" >1.1276259652063806981…</td><td align="center" valign="middle" >3.510e−03</td></tr><tr><td align="center" valign="middle" >0.6</td><td align="center" valign="middle" >1.18179111195371…</td><td align="center" valign="middle" >1.1854652182422675821…</td><td align="center" valign="middle" >3.674e−03</td></tr><tr><td align="center" valign="middle" >0.7</td><td align="center" valign="middle" >1.25166573656183…</td><td align="center" valign="middle" >1.2551690056309430243…</td><td align="center" valign="middle" >3.503e−03</td></tr><tr><td align="center" valign="middle" >0.8 0.9</td><td align="center" valign="middle" >1.33452729205395… 1.43130499800870…</td><td align="center" valign="middle" >1.3374349463048447184… 1.4330863854487745356…</td><td align="center" valign="middle" >2.907e−03 1.781e−03</td></tr></tbody></table></table-wrap><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> Error comparisons for solving the problem of ODE (37).</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/6-1720726x114.png"/></fig></fig-group></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we construct a group of iterative methods with cubic convergence for the systems of nonlinear equations by using the Gauss-Legendre quadrature formula. Numerical results we gave are in consistence with the theoretical analysis, and meanwhile they also demonstrate that the presented scheme is efficient and feasible to solve systems of nonlinear equations and to solve two-point boundary-value problems of nonlinear ordinary differential equations.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The work is supported by the Science and Technology Program of Beijing Municipal Commission of Education (No. KM201511417012).</p></sec><sec id="s6"><title>Cite this paper</title><p>Liu, Z.L. and Sun, G.Q. (2016) Gauss-Legendre Iterative Methods and Their Applications on Nonlinear Systems and BVP-ODEs. 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