<?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.2015.310154</article-id><article-id pub-id-type="publisher-id">JAMP-60679</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>
 
 
  A New Newton-Type Method with Third-Order for Solving Systems of Nonlinear Equations
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>hongli</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Quanyou</surname><given-names>Fang</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>College of Biochemical Engineering, Beijing Union University, Beijing, China</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>liuzhongli2@163.com(HL)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>20</day><month>10</month><year>2015</year></pub-date><volume>03</volume><issue>10</issue><fpage>1256</fpage><lpage>1261</lpage><history><date date-type="received"><day>12</day>	<month>September</month>	<year>2015</year></date><date date-type="rev-recd"><day>accepted</day>	<month>25</month>	<year>October</year>	</date><date date-type="accepted"><day>28</day>	<month>October</month>	<year>2015</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
 
 
  In this paper, a new two-step Newton-type method with third-order convergence for solving systems of nonlinear equations is proposed. We construct the new method based on the integral interpolation of Newton’s method. Its cubic convergence and error equation are proved theoretically, and demonstrated numerically. Its application to systems of nonlinear equations and boundary-value problems of nonlinear ODEs are shown as well in the numerical examples.
 
</p></abstract><kwd-group><kwd>Newton-Type Method</kwd><kwd> Systems of Nonlinear Equations</kwd><kwd> Third-Order Convergence</kwd><kwd> Integral Interpolation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>We consider a system of nonlinear equations as follows:</p><disp-formula id="scirp.60679-formula1393"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x6.png"  xlink:type="simple"/></disp-formula><p>where, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x7.png" xlink:type="simple"/></inline-formula>is a given nonlinear function with the following properties:</p><p>1) There exists an <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x8.png" xlink:type="simple"/></inline-formula> such that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x9.png" xlink:type="simple"/></inline-formula>;</p><p>2) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x10.png" xlink:type="simple"/></inline-formula>is continuously differentiable in a neighborhood of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x11.png" xlink:type="simple"/></inline-formula>;</p><p>3) <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x12.png" xlink:type="simple"/></inline-formula>is a nonsingular matrix.</p><p>How to efficiently solve the system of nonlinear Equation (1) is a typical issue in scientific computation and engineering field. The most famous method is probably Newton’s method as follows (see [<xref ref-type="bibr" rid="scirp.60679-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.60679-ref2">2</xref>] ):</p><disp-formula id="scirp.60679-formula1394"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x13.png"  xlink:type="simple"/></disp-formula><p>where x<sub>0</sub> is an initial guess of the root. This is one-step method, and it uses two evaluations of the function and derivative to achieve second-order convergence by iteration.</p><p>Besides, third-order iterative equations, such as the Halley iterative method and Chebyshev iterative method, are often used. In recent years, a few similar methods [<xref ref-type="bibr" rid="scirp.60679-ref3">3</xref>] -[<xref ref-type="bibr" rid="scirp.60679-ref9">9</xref>] with high-order have emerged for solving systems of nonlinear equations.</p><p>Especially, M. T. Darvish &amp; A. Barati [<xref ref-type="bibr" rid="scirp.60679-ref3">3</xref>] used Adomian decomposition method to construct a third-order Newton-type scheme:</p><disp-formula id="scirp.60679-formula1395"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x14.png"  xlink:type="simple"/></disp-formula><p>Frontini &amp; Sormani [<xref ref-type="bibr" rid="scirp.60679-ref4">4</xref>] presented a third-order method in using numerical quadrature formulae to solve systems of nonlinear equations as follows:</p><disp-formula id="scirp.60679-formula1396"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x15.png"  xlink:type="simple"/></disp-formula><p>These are classic two-step Newton-type methods to achieve cubic convergence to approximate the root of a system of nonlinear equations.</p><p>In this paper, we propose a new variant of two-step Newton’s method with the third-order convergence by quadrature formulae in Section 2, some numerical examples using this new method for solving systems of nonlinear equations and boundary-value problems of nonlinear ODEs in Section 3, and finally make conclusions in Section 4.</p></sec><sec id="s2"><title>2. The New Method and Its Third-Order Convergence</title><p>Based on the multivariable mean-value theorem</p><disp-formula id="scirp.60679-formula1397"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x16.png"  xlink:type="simple"/></disp-formula><p>we use the left rectangular integral rule</p><disp-formula id="scirp.60679-formula1398"><graphic  xlink:href="http://html.scirp.org/file/5-1720372x17.png"  xlink:type="simple"/></disp-formula><p>and use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x18.png" xlink:type="simple"/></inline-formula> to get Newton Method (1). By using the trapezoidal integral rule</p><disp-formula id="scirp.60679-formula1399"><graphic  xlink:href="http://html.scirp.org/file/5-1720372x19.png"  xlink:type="simple"/></disp-formula><p>substituting <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x20.png" xlink:type="simple"/></inline-formula> with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x21.png" xlink:type="simple"/></inline-formula>, and using<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x22.png" xlink:type="simple"/></inline-formula>, Weerakoon and Fernando [<xref ref-type="bibr" rid="scirp.60679-ref5">5</xref>] also derived a variant of Newton’s method with cubic convergence (3) for a nonlinear equation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x23.png" xlink:type="simple"/></inline-formula>.</p><p>Now, we applied the quadrature formula</p><disp-formula id="scirp.60679-formula1400"><graphic  xlink:href="http://html.scirp.org/file/5-1720372x24.png"  xlink:type="simple"/></disp-formula><p>to construct the following new scheme:</p><disp-formula id="scirp.60679-formula1401"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x25.png"  xlink:type="simple"/></disp-formula><p>We state and prove the convergence theorem as follows:</p><p>Theorem Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x26.png" xlink:type="simple"/></inline-formula> be 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/5-1720372x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x27.png" xlink:type="simple"/></inline-formula> and x<sub>0</sub> be close to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x28.png" xlink:type="simple"/></inline-formula>, then the new of Newton-type method (6) is cubically convergent, and its error equation is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x29.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. As<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x30.png" xlink:type="simple"/></inline-formula>, and note<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x31.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x30.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x31.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x32.png" xlink:type="simple"/></inline-formula>.</p><p>By Taylor’s expansion, we have</p><disp-formula id="scirp.60679-formula1402"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x33.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.60679-formula1403"><label>, (8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x34.png"  xlink:type="simple"/></disp-formula><p>From</p><disp-formula id="scirp.60679-formula1404"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x35.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x36.png" xlink:type="simple"/></inline-formula> is sufficiently small.</p><p>We have</p><disp-formula id="scirp.60679-formula1405"><graphic  xlink:href="http://html.scirp.org/file/5-1720372x37.png"  xlink:type="simple"/></disp-formula><p>By (6), therefore</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x38.png" xlink:type="simple"/></inline-formula>.</p><p>And</p><disp-formula id="scirp.60679-formula1406"><graphic  xlink:href="http://html.scirp.org/file/5-1720372x39.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x40.png" xlink:type="simple"/></inline-formula>.</p><p>By Toylor’s expansion</p><disp-formula id="scirp.60679-formula1407"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x41.png"  xlink:type="simple"/></disp-formula><p>Furthermore, by (8) and (10), we have</p><disp-formula id="scirp.60679-formula1408"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x42.png"  xlink:type="simple"/></disp-formula><p>Finally, using (7), (11) and (6), we obtain the error equation as</p><disp-formula id="scirp.60679-formula1409"><graphic  xlink:href="http://html.scirp.org/file/5-1720372x43.png"  xlink:type="simple"/></disp-formula><p>That is</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x44.png" xlink:type="simple"/></inline-formula>.</p><p>Using (9), so,</p><disp-formula id="scirp.60679-formula1410"><label>. (12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x45.png"  xlink:type="simple"/></disp-formula><p>This shows that the method is the third-order convergence.</p><p>The new scheme of two-step Newton-type method (6) uses three evaluations of the function and derivative per iteration to achieve third-order convergence for solving a simple root of systems of nonlinear equations. As the efficiency index is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x46.png" xlink:type="simple"/></inline-formula>, the efficiency index of the Newton-type method is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x47.png" xlink:type="simple"/></inline-formula>, whereas Newton’s method is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x48.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s3"><title>3. Numerical Examples</title><p>The iterative method (6) is demonstrated by solving some systems of nonlinear equations and boundary-value problems of nonlinear ODE.</p><p>Example 1. Consider the system of nonlinear equation:</p><disp-formula id="scirp.60679-formula1411"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x49.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x50.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x51.png" xlink:type="simple"/></inline-formula>. We have numerical results in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>According to results of the numerical experiments, the new iterative method (6) can achieve super third-order convergence for some systems of nonlinear equations.</p><p>Example 2. We have numerical results in <xref ref-type="table" rid="table2">Table 2</xref> for the following a system of nonlinear equations:</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> The solutions and errors of the system of Equations (13) using method (6)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x52.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x53.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x54.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x55.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x56.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3.444444444444444039576788</td><td align="center" valign="middle" >−1.025641025641025617667891</td><td align="center" valign="middle" >1.446e−0</td><td align="center" valign="middle" >1.971e−0</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1.999998516331195414738740</td><td align="center" valign="middle" >−0.9999996492101374900753236</td><td align="center" valign="middle" >1.524e−6</td><td align="center" valign="middle" >1.854e−6</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2.000000000000000000004496</td><td align="center" valign="middle" >−1.0000000000000000000008992</td><td align="center" valign="middle" >4.585e−21</td><td align="center" valign="middle" >5.395e−21</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1.999999999999999999999999</td><td align="center" valign="middle" >−0.999999999999999999999999</td><td align="center" valign="middle" >7.725e−65</td><td align="center" valign="middle" >9.091e−65</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The solutions of the system of Equations (14) using method (6)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x57.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x58.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x59.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x60.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x61.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.499565371550889536</td><td align="center" valign="middle" >0.006147092477281110</td><td align="center" valign="middle" >−0.521628814405284191</td><td align="center" valign="middle" >1.07e−1</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.500000035199424988</td><td align="center" valign="middle" >0.000005327105559032</td><td align="center" valign="middle" >−0.523598502730812839</td><td align="center" valign="middle" >8.61e−5</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.500000000000000033</td><td align="center" valign="middle" >0.000000000000003291</td><td align="center" valign="middle" >−0.523598775598308161</td><td align="center" valign="middle" >1.97e−13</td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0.500000000000000000</td><td align="center" valign="middle" >0.000000000000000000</td><td align="center" valign="middle" >−0.523598775598298873</td><td align="center" valign="middle" >1.09e−31</td></tr></tbody></table></table-wrap><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> The errors of the system of Equations (16) using method (6)</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x62.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/5-1720372x63.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.439e−2</td><td align="center" valign="middle" >1.238e−10</td><td align="center" valign="middle" >1.612e−14</td><td align="center" valign="middle" >1.612e−14</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x64.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.996e−3</td><td align="center" valign="middle" >6.128e−12</td><td align="center" valign="middle" >7.926e−37</td><td align="center" valign="middle" >1.729e−112</td></tr></tbody></table></table-wrap><p><sup>*</sup>Corresponding author.</p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x66.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x66.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x67.png" xlink:type="simple"/></inline-formula>.</p><p>The above numerical results agree with the theoretical analysis on the convergence, and the iterative efficiency is comparative high.</p><p>Example 3. Consider solving the following boundary-value problem of nonlinear ODE:</p><disp-formula id="scirp.60679-formula1412"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x68.png"  xlink:type="simple"/></disp-formula><p>Discretize the nonlinear ODE (15) with the finite difference method. Taking nodes<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x69.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x70.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x69.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x71.png" xlink:type="simple"/></inline-formula>, we have a system of nine-dimensional nonlinear equations:</p><disp-formula id="scirp.60679-formula1413"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/5-1720372x72.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x73.png" xlink:type="simple"/></inline-formula>, using the Newton-type method (6), we get the solutions <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x73.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/5-1720372x74.png" xlink:type="simple"/></inline-formula> of Equations (16), that is</p><disp-formula id="scirp.60679-formula1414"><graphic  xlink:href="http://html.scirp.org/file/5-1720372x75.png"  xlink:type="simple"/></disp-formula><p>The results for the system of nonlinear equations of ODE (15) are shown in <xref ref-type="table" rid="table3">Table 3</xref>.</p></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, we presented a new two-step iterative method of cubic convergence to solve systems of nonlinear equations. Through theoretical analysis and numerical experiments, we believe that the new variant of Newton- type method is so efficient and fast convergent as to be able to find solutions with required accuracy. To sum up, this method is suitable for solving systems of nonlinear equations, and can be used to resolve boundary-value problems of nonlinear ordinary differential equations as well.</p></sec><sec id="s5"><title>Acknowledgements</title><p>The work is funded by the Science &amp; Technology Program of Beijing Municipal Commission of Education (No. KM201511417012).</p></sec><sec id="s6"><title>Cite this paper</title><p>ZhongliLiu,QuanyouFang, (2015) A New Newton-Type Method with Third-Order for Solving Systems of Nonlinear Equations. Journal of Applied Mathematics and Physics,03,1256-1261. doi: 10.4236/jamp.2015.310154</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.60679-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ortega, J.M. and Rheinboldt, W.G. (1970) Iterative Solution of Nonlinear Equations in Several Variables. Academic Press, New York.</mixed-citation></ref><ref id="scirp.60679-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Traub, J.F. (1964) Iterative Methods for the Solution of Equations. Prentice-Hall, Englewood Cliffs, New Jer-sey.</mixed-citation></ref><ref id="scirp.60679-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Darvish, M.T. and Barati, A. (2007) A Third-Order Newton-Type Method to Solve Systems of Nonlinear Equations. 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