<?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.2017.87073</article-id><article-id pub-id-type="publisher-id">AM-77655</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>
 
 
  Simpson’s Method for Solution of Nonlinear Equation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hamideh</surname><given-names>Eskandari</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 Mathematics, Payame Noor University, Tehran, Iran</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>h_eskandari@pnu.ac.ir</email></corresp></author-notes><pub-date pub-type="epub"><day>03</day><month>07</month><year>2017</year></pub-date><volume>08</volume><issue>07</issue><fpage>929</fpage><lpage>933</lpage><history><date date-type="received"><day>5,</day>	<month>June</month>	<year>2017</year></date><date date-type="rev-recd"><day>11,</day>	<month>July</month>	<year>2017</year>	</date><date date-type="accepted"><day>14,</day>	<month>July</month>	<year>2017</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>
 
 
  The programs offered for solving nonlinear equations, usually the old method, such as alpha, chordal movement, Newton, etc. have been used. Among these methods may Newton’s method of them all be better and higher integration. In this paper, we propose the integration method for finding the roots of nonlinear equation we use. In this way, Newton’s method uses integration methods to obtain. In previous work, [1] and [2] presented numerical integration methods such as integration, trapezoidal and rectangular integration method that are used. The new method proposed here, uses Simpson’s integration. With this method, the approximation error is reduced. The calculated results show that this hypothesis is confirmed.
 
</p></abstract><kwd-group><kwd>Convergence</kwd><kwd> Newton Method</kwd><kwd> Simpson Method</kwd><kwd> Nonlinear Equation</kwd><kwd> Iterative Method</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Let f : R → R be a smooth nonlinear function with a simple root x * , i.e. f ( x * ) = 0 and f ′ ( x * ) ≠ 0. . We consider iterative methods for the calculation of x * that uses f and f ′ but not the higher derivatives of f and that generalizes the Newton method. Modifications for multiple roots will not be considered in the present contribution.</p><p>To find the roots of an equation of nonlinear methods, there are many methods. Most famous method to find the approximate root of x * from the equation, non-linear and using the first derivative, is what called Newton’s method. ( [<xref ref-type="bibr" rid="scirp.77655-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.77655-ref8">8</xref>] ).</p><p>We know that Newton’s method, an iterative procedure is to obtain an approximate root of the equation f ( x ) = 0 , with an initial guess x 0 ∈ R , for n = 0 , 1 , 2 , ⋯ values</p><p>x n + 1 = x n − f ( x n ) f ′ ( x n ) (1)</p><p>Calculates show that this formula is repeated, with the convergence of order two.</p></sec><sec id="s2"><title>2. Elementarily Methods</title><p>Newton’s iteration formula in different ways and in many ways can be found [<xref ref-type="bibr" rid="scirp.77655-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.77655-ref8">8</xref>] . But in this paper specific integration methods, we use. According to the definite integral</p><p>∫ x n x f ′ ( t ) d t = f ( x ) − f ( x n ) (2)</p><p>can write</p><p>f ( x ) = f ( x n ) + ∫ x n x f ′ ( t ) d t (3)</p><p>The definite integral in this regard can be calculated by different methods. If this is the definite integral of the square method [<xref ref-type="bibr" rid="scirp.77655-ref1">1</xref>] to obtain, can be written</p><p>∫ x n x f ′ ( t ) d t ≅ ( x − x n ) f ′ ( x n ) (4)</p><p>After placement in relation to certain integration, we get the following statement.</p><p>f ( x ) ≅ f ( x n ) + ( x − x n ) f ′ ( x n ) (5)</p><p>According to f ( x ) = 0 is due to the new value x = x n − f ( x n ) f ′ ( x n ) to obtain</p><p>the same formula is repeated Newton [<xref ref-type="bibr" rid="scirp.77655-ref9">9</xref>] .</p><p>As well as to find solutions integrator can be used as [<xref ref-type="bibr" rid="scirp.77655-ref1">1</xref>] of midpoint method.</p><p>∫ x n x f ′ ( t ) d t ≅ ( x − x n ) f ′ ( x n + x 2 ) (6)</p><p>And with Placement x = x n − f ( x n ) f ′ ( x n ) that is Newton iteration, to new itera-</p><p>tion will reach a formula.</p><p>x n + 1 = x n − f ( x n ) f ′ ( x n − f ( x n ) 2 f ′ ( x n ) ) (7)</p><p>However, if we use trapezoidal method and midpoint method instead of rectangular method [<xref ref-type="bibr" rid="scirp.77655-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.77655-ref2">2</xref>] , then the method can be written</p><p>∫ x n x f ′ ( t ) d t ≅ ( x − x n ) 2 [ f ′ ( x n ) + f ′ ( x ) ] (8)</p><p>And the placement of certain integration, we get the following statement.</p><p>f ( x ) ≅ f ( x n ) + ( x − x n ) 2 [ f ′ ( x n ) + f ′ ( x ) ] (9)</p><p>And according to f ( x ) = 0 is the new value of x = x n − 2 f ( x n ) [ f ′ ( x n ) + f ′ ( x ) ] to obtain by replacing f ′ ( x ) with f ′ ( x n + 1 ) , where x n + 1 = x n − f ( x n ) f ′ ( x n ) is New-</p><p>ton repeated the following three methods to obtain explicit order.</p><p>x n + 1 = x n − 2 f ( x n ) f ′ ( x n ) + f ′ ( x n − f ( x n ) f ′ ( x n ) ) (10)</p><p>This relationship, modified Newton iteration formula [<xref ref-type="bibr" rid="scirp.77655-ref10">10</xref>] is.</p></sec><sec id="s3"><title>3. Preliminary Results</title><p>Now back to the original Equation (3) return.</p><p>To find the definite integral in the above equation, we use the method of Simpson [<xref ref-type="bibr" rid="scirp.77655-ref3">3</xref>] . We can write</p><p>∫ x n x f ′ ( t ) d t = x − x n 2 3 ( f ′ ( x ) + 4 f ′ ( x + x n 2 ) + f ′ ( x n ) ) (11)</p><p>By substituting the equation can be written</p><p>f ( x ) = f ( x n ) + x − x n 6 ( f ′ ( x ) + 4 f ′ ( x + x n 2 ) + f ′ ( x n ) ) (12)</p><p>According to the f ( x ) = 0 , we will gain new value</p><p>x = x n − 6 f ( x n ) [ f ′ ( x ) + 4 f ′ ( x + x n 2 ) + f ′ ( x n ) ] and substitution x with x n + 1 explicit method to obtain, where in x n + 1 = x n − f ( x n ) f ′ ( x n ) is Newton method.</p><p>x n + 1 = x n − 6 f ( x n ) [ f ′ ( x n − f ( x n ) f ′ ( x n ) ) + 4 f ′ ( x n − f ( x n ) f ′ ( x n ) + x n 2 ) + f ′ ( x n ) ]</p><p>And then we’ll simplify.</p><p>x n + 1 = x n − 6 f ( x n ) [ f ′ ( x n − f ( x n ) f ′ ( x n ) ) + 4 f ′ ( x n − f ( x n ) 2 f ′ ( x n ) ) + f ′ ( x n ) ] (13)</p><p>This relationship, a new iterative method is a convergence of order higher than two.</p><p>Methods that have already been presented, rectangular and trapezoidal integration method is used. These methods have convergence times lower than Simpson’s method. In the future we will see that this method is superior to other methods and convergence is it better than before.</p><p>Here, all computing software Maple is done and we have one of the following stop conditions:</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Example 1</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x41.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x42.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x43.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >1.6504206952163954715</td><td align="center" valign="middle" >0.34641095924425665672</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >1.9305183053827568405</td><td align="center" valign="middle" >0.00547642190321585418</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >1.9345632028456436684</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x44.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >1.9345632107520242676</td><td align="center" valign="middle" >0.</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >1.9345632107520242676</td><td align="center" valign="middle" >0.</td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Example 2</title></caption><table><tbody><thead><tr><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x45.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x46.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x47.png" xlink:type="simple"/></inline-formula></th></tr></thead><tr><td align="center" valign="middle" >1</td><td align="center" valign="middle" >0.78027135582726141440</td><td align="center" valign="middle" >0.01676581394101499529</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >0.77288330212111547221</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x48.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >0.77288295914921011288</td><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-7403630x49.png" xlink:type="simple"/></inline-formula></td></tr><tr><td align="center" valign="middle" >4</td><td align="center" valign="middle" >0.77288295914921011285</td><td align="center" valign="middle" >0.</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >0.77288295914921011285</td><td align="center" valign="middle" >0.</td></tr></tbody></table></table-wrap><p>(I) | x n + 1 − x n | &lt; ε</p><p>(II) | f ( x n + 1 ) | &lt; ε</p><p>In each of them ε = 10 − 1000 and also all computations were done using Maple using 128 digit floating point arithmetic (Digits: = 128).</p></sec><sec id="s4"><title>4. Numerical Experiments</title><p>In this section, we will test several functions in obtained iteration formula.</p><p>Example 1:</p><p>Consider the equation f ( x ) = sin x − x + 1 = 0 . Starting from the point x 0 = 1.0 , we obtain the value of 1 .9345632107520242676 , if 1 .9345632107520242676 is the exact answer. Different iterations of this method in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Example 2:</p><p>Consider the equation f ( x ) = x 3 − e − x = 0 . Starting from the point x 0 = 1.0 , we obtain the value of 0 .77288295914921011285 , if 0 .77288295914921011285 is the exact answer. Different iterations of this method in <xref ref-type="table" rid="table2">Table 2</xref>.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, to solve a nonlinear equation formula offered new iteration, we have seen that this formula iteration was obtained using Simpson integration. It was observed that using examples provided, its accuracy is higher than the accuracy of Newton iterative method.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This article is supported by Payame Noor University.</p></sec><sec id="s7"><title>Cite this paper</title><p>Eskandari, H. (2017) Simpson’s Method for Solution of Nonlinear Equation. Applied Mathematics, 8, 929-933. https://doi.org/10.4236/am.2017.87073</p></sec></body><back><ref-list><title>References</title><ref id="scirp.77655-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Frontini, M. and Sormani, E. (2003) Some Variant of Newton’s Method with Third-Order Convergence. Applied Mathematics and Computation, 140, 419-426.  
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