<?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.2016.76043</article-id><article-id pub-id-type="publisher-id">AM-64928</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 Approach for Solving Nonlinear Equations by Using of Integer Nonlinear Programming
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>rmin</surname><given-names>Ghane-Kanafi</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>Sohrab</surname><given-names>Kordrostami</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Lahijan Branch, Islamic Azad University, Lahijan, Iran</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>arminghane@liau.ac.ir(RG)</email>;<email>krostami@liau.ac.ir(SK)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>24</day><month>03</month><year>2016</year></pub-date><volume>07</volume><issue>06</issue><fpage>473</fpage><lpage>481</lpage><history><date date-type="received"><day>17</day>	<month>January</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>21</month>	<year>March</year>	</date><date date-type="accepted"><day>24</day>	<month>March</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><html>
 <head></head>
 
  One of the most important issues in numerical calculations is finding simple roots of nonlinear equations. This topic is one of the oldest challenges in science and engineering. Many important problems in engineering, to achieve the result need to solve a nonlinear equation. Thus, the formulation of a recursive relationship with high order of convergence and low time complexity is very important. This paper provides a modification to the Weerakoon-Fernando and Parhi-Gupta methods. It is shown that, in each iterate, the improved method requires three evaluations of the function and two evaluations of the first derivatives of function. The proposed with the Kou et al., Neta, Parhi-Gupta, Thukral and Mir et al. methods have been applied to a collection of 12 test problem. The results show that proposed approach significantly reduces the number of function calls when compared to the above methods. The numerical examples show that the proposed method is more efficiency than other methods in this class, such as sixth-order method of Parhi-Gupta or eighth-order method of Mir et al. and Thukral. We show that the order of convergence the proposed method is 9 and also, the modified method has the efficiency of 
  <img src="Edit_00198af3-01d6-4fc4-b759-14b776cee18f.bmp" alt="" />.
 
</html></p></abstract><kwd-group><kwd>Newton Method</kwd><kwd> Nonlinear Equations</kwd><kwd> Convergence Theorem</kwd><kwd> Efficiency Index</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In the real world, many of the complex problems after simplification lead to solving nonlinear problems. Find an approximation of the simple roots of the equations is one of the important problems on this issue. The rapid development of technology has led to different of algorithms. Over time, many algorithms have been developed. In this state, one of the ways for comparison of different algorithms is finding of complexity of time and index efficiency of algorithms. MAPLE software is one of the powerful algebraic systems from Maplesoft company, such that in this article it has been used for the calculation. The boundary value problems appearing in kinetic theory of gases, elasticity and other applied areas are reduced to solve these equations. Many optimization problems also lead such equations. Hence, one of the most important problems in numerical analysis is to find a simple root a of a nonlinear equation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x7.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x8.png" xlink:type="simple"/></inline-formula> for an open interval <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x9.png" xlink:type="simple"/></inline-formula> is a scalar function. In this study, in order to find a, we should start with an initial approximation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x10.png" xlink:type="simple"/></inline-formula> which is near to the root and generates successive iterates <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x11.png" xlink:type="simple"/></inline-formula> converging to simple root a of nonlinear equation<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x12.png" xlink:type="simple"/></inline-formula>. In all iteration, the improved method requires three evaluations of the function and two evaluations of the first order derivatives of function. Therefore, the modified method has the efficiency index<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x13.png" xlink:type="simple"/></inline-formula>. The numerical examples show that, the proposed method has more efficient with respect to the Newton method and other methods in this class. The effectiveness of the modified ninth-order method will be examined by approximation the simple root of a given non-linear equation. The suggested method is comparable to the sixth-order methods [<xref ref-type="bibr" rid="scirp.64928-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.64928-ref2">2</xref>] ; also the eighth-order methods [<xref ref-type="bibr" rid="scirp.64928-ref3">3</xref>] and [<xref ref-type="bibr" rid="scirp.64928-ref4">4</xref>] .</p><p>In the reminder, we proceed as follows: In Section 2, we recall the basic concepts. The proposed method is described in Section 3. In Section 4, the convergence analysis is carried out to establish the ninth-order of convergence of our method. In Section 5, as is shown in the numerical examples, this method is more efficient than Newton method and other methods of lower or same order. We conclude with some remarks on the presented approaches in Section 6.</p></sec><sec id="s2"><title>2. Several Basic Definitions</title><p>Our goal is to find the value of x that satisfies the following equation.</p><disp-formula id="scirp.64928-formula425"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x14.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x15.png" xlink:type="simple"/></inline-formula> is a nonlinear equation. The value of x that satisfies (1) is called a root of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x16.png" xlink:type="simple"/></inline-formula> and denoted by a. Therefore, the procedure used of to find x is called root-finding. Let a is a simple root of Equation (1) and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x17.png" xlink:type="simple"/></inline-formula> is a real sequence.</p><p>Definition 1. See [<xref ref-type="bibr" rid="scirp.64928-ref5">5</xref>] : The sequence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x18.png" xlink:type="simple"/></inline-formula> is said to converge to a if</p><disp-formula id="scirp.64928-formula426"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x19.png"  xlink:type="simple"/></disp-formula><p>Furthermore, if there exists positive constant c and p such that:</p><disp-formula id="scirp.64928-formula427"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x20.png"  xlink:type="simple"/></disp-formula><p>we say that <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x21.png" xlink:type="simple"/></inline-formula> converges to a of order p. Larger values of p correspond to faster convergence. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x22.png" xlink:type="simple"/></inline-formula> be error in the nth iterate of the method which produces the sequence<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x23.png" xlink:type="simple"/></inline-formula>. The relation</p><disp-formula id="scirp.64928-formula428"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x24.png"  xlink:type="simple"/></disp-formula><p>is called the error equation. The value of p is called the order of convergence of method, see [<xref ref-type="bibr" rid="scirp.64928-ref6">6</xref>] .</p><p>Definition 2. Let a be a root of the function f and suppose that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x25.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x26.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x27.png" xlink:type="simple"/></inline-formula> are three consecutive iterations closer to the root a. The the computational order of convergence <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x28.png" xlink:type="simple"/></inline-formula> can be approximated using the formula:</p><disp-formula id="scirp.64928-formula429"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x29.png"  xlink:type="simple"/></disp-formula></sec><sec id="s3"><title>3. New Proposed Scheme</title><p>The new method is based on [<xref ref-type="bibr" rid="scirp.64928-ref2">2</xref>] method. With a simple manipulation, and a new approach to get the following equations.</p><disp-formula id="scirp.64928-formula430"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x30.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula431"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x31.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula432"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x32.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.64928-formula433"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x33.png"  xlink:type="simple"/></disp-formula><p>This is four-step method. It is not necessary to compute the first-order derivative at the point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x34.png" xlink:type="simple"/></inline-formula> since a good approximation can be obtained. In order to approximate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x35.png" xlink:type="simple"/></inline-formula> use the linear interpolation on two points <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x36.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x37.png" xlink:type="simple"/></inline-formula>, so we have:</p><disp-formula id="scirp.64928-formula434"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x38.png"  xlink:type="simple"/></disp-formula><p>Therefore,</p><disp-formula id="scirp.64928-formula435"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x39.png"  xlink:type="simple"/></disp-formula><p>Now using Equations (2), we have:</p><disp-formula id="scirp.64928-formula436"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x40.png"  xlink:type="simple"/></disp-formula><p>Substituting the relation of (6) into the relation (3), in this case, we obtain the following formula:</p><disp-formula id="scirp.64928-formula437"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula438"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x42.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula439"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x43.png"  xlink:type="simple"/></disp-formula><p>where,</p><disp-formula id="scirp.64928-formula440"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x44.png"  xlink:type="simple"/></disp-formula><p>Obviously this method requires evaluations of three function f and two derivatives<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x45.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s4"><title>4. Convergence Analysis</title><p>To determine order of convergence of proposed method, we must be solving integer nonlinear programming as follow:</p><disp-formula id="scirp.64928-formula441"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x46.png"  xlink:type="simple"/></disp-formula><p>where C is a special coefficient of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x47.png" xlink:type="simple"/></inline-formula>. This is equivalent to the bellow theorem, i.e. we show that the convergence of the proposed method is of the order of 9.</p><p>Theorem 1. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x49.png" xlink:type="simple"/></inline-formula> has continuous derivative function and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x50.png" xlink:type="simple"/></inline-formula> is a simple root of f. If the initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x50.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x51.png" xlink:type="simple"/></inline-formula> is sufficiently close1 to a, then the method defined by (2) converges to a in the ninth-order. Furthermore, the error in the method given by (2) satisfies the equation:</p><disp-formula id="scirp.64928-formula442"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x52.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x53.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x54.png" xlink:type="simple"/></inline-formula> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x53.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x55.png" xlink:type="simple"/></inline-formula>.</p><p>Proof. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x56.png" xlink:type="simple"/></inline-formula> be the error term in the iterate<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x57.png" xlink:type="simple"/></inline-formula>. Using Taylor expansion, we have:</p><disp-formula id="scirp.64928-formula443"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x58.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.64928-formula444"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x59.png"  xlink:type="simple"/></disp-formula><p>Quotient relations (9) and (10), gives the following results:</p><disp-formula id="scirp.64928-formula445"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x60.png"  xlink:type="simple"/></disp-formula><p>Thus we have</p><disp-formula id="scirp.64928-formula446"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x61.png"  xlink:type="simple"/></disp-formula><p>Taylor expansion of the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x62.png" xlink:type="simple"/></inline-formula> around the point a to get the following result (i.e (11)):</p><disp-formula id="scirp.64928-formula447"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x63.png"  xlink:type="simple"/></disp-formula><p>Substituting (9), (10) and (11) into the z<sub>n</sub> section of the Equation (2), we have:</p><disp-formula id="scirp.64928-formula448"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x64.png"  xlink:type="simple"/></disp-formula><p>Furthermore, the Taylor expansion of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x65.png" xlink:type="simple"/></inline-formula> about a is</p><disp-formula id="scirp.64928-formula449"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x66.png"  xlink:type="simple"/></disp-formula><p>Since from (10), (12) and (13) we get:</p><disp-formula id="scirp.64928-formula450"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x67.png"  xlink:type="simple"/></disp-formula><p>Again, using the Taylor expansion of function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x68.png" xlink:type="simple"/></inline-formula> about the point a, in this case we have:</p><disp-formula id="scirp.64928-formula451"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x69.png"  xlink:type="simple"/></disp-formula><p>Taylor expansion of the function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x70.png" xlink:type="simple"/></inline-formula> around the point a to get the following result (i.e (16)):</p><disp-formula id="scirp.64928-formula452"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x71.png"  xlink:type="simple"/></disp-formula><p>In this case, using the above result (i.e (15), (16) and (14)) and corresponding to the relation (3), we get:</p><disp-formula id="scirp.64928-formula453"><label>(17)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/3-7403060x72.png"  xlink:type="simple"/></disp-formula><p>Therefore, we have:</p><disp-formula id="scirp.64928-formula454"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x73.png"  xlink:type="simple"/></disp-formula><p>Thus, the ninth order of convergence of the method is established.</p>Numerical Examples<p>In order to demonstrate the performance, accuracy and effectiveness of the proposed ninth-order method, we take 12 special nonlinear equation test problems from [<xref ref-type="bibr" rid="scirp.64928-ref2">2</xref>] [<xref ref-type="bibr" rid="scirp.64928-ref7">7</xref>] and [<xref ref-type="bibr" rid="scirp.64928-ref8">8</xref>] . We compare the proposed method with Wang-Liu’s third-order method [<xref ref-type="bibr" rid="scirp.64928-ref8">8</xref>] , Weerakoon-Fernando and Parhi-Gupta’s sixth-order methods [<xref ref-type="bibr" rid="scirp.64928-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.64928-ref2">2</xref>] and Kou et al. and Neta’s eight-order methods as [<xref ref-type="bibr" rid="scirp.64928-ref3">3</xref>] and [<xref ref-type="bibr" rid="scirp.64928-ref4">4</xref>] , respectively. The computing results displayed in Tables 1-5. In every problem we try to seek an approximation <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x74.png" xlink:type="simple"/></inline-formula> of the root a of Equation (1) after n times</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Comparison of result of proposed method (PM) with Kou and Li (KL) method</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Functions</th><th align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x75.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  >n</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >Run time</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >NFE</th></tr></thead><tr><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >KL</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >KL</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >KL</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x76.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.031</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >36</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.032</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >32</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x77.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.390</td><td align="center" valign="middle" >0.468</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >64</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.421</td><td align="center" valign="middle" >0.343</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >36</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x78.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.187</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >32</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >128</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x79.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.265</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >36</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >13</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >0.016</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >52</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x80.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >68</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.406</td><td align="center" valign="middle" >0.312</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >272</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.484</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x81.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >84</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x82.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.234</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x83.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >163</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >652</td></tr><tr><td align="center" valign="middle" >4.5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >433</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.343</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >1732</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x84.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.296</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x85.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.468</td><td align="center" valign="middle" >0.312</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >40</td></tr><tr><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.515</td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >24</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x86.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.85</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.827</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.577</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x87.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >23</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.171</td><td align="center" valign="middle" >0.031</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >92</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >51</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.281</td><td align="center" valign="middle" >0.016</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >204</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 result of proposed method (PM) with Parhi and Gupta (PG) method</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Functions</th><th align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x88.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  >n</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >Run time</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >NFE</th></tr></thead><tr><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >PG</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >PG</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >PG</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x89.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.031</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.093</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x90.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.390</td><td align="center" valign="middle" >0.218</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.421</td><td align="center" valign="middle" >0.312</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x91.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.187</td><td align="center" valign="middle" >0.124</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >44</td></tr><tr><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" >0.031</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x92.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.265</td><td align="center" valign="middle" >0.094</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >0.078</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x93.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.406</td><td align="center" valign="middle" >0.250</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.484</td><td align="center" valign="middle" >0.265</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x94.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.047</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x95.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.234</td><td align="center" valign="middle" >0.172</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >0.141</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x96.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >4.5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.140</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >28</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x97.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.296</td><td align="center" valign="middle" >0.063</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x98.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.468</td><td align="center" valign="middle" >0.312</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.515</td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x99.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.85</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.827</td><td align="center" valign="middle" >0.656</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >60</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.577</td><td align="center" valign="middle" >0.250</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x100.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.171</td><td align="center" valign="middle" >0.078</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.281</td><td align="center" valign="middle" >0.062</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >20</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 result of proposed method (PM) with Neta (NM) method</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Functions</th><th align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x101.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  >n</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >Run time</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >NFE</th></tr></thead><tr><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >NM</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >NM</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >NM</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x102.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.109</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x103.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.390</td><td align="center" valign="middle" >0.312</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.421</td><td align="center" valign="middle" >0.374</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x104.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.187</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" >0.094</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x105.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.265</td><td align="center" valign="middle" >0.124</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >0.093</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x106.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.406</td><td align="center" valign="middle" >0.390</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.484</td><td align="center" valign="middle" >0.437</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x107.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.141</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x108.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.234</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >0.141</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x109.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.093</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" >4.5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >28</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x110.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.296</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x111.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.468</td><td align="center" valign="middle" >0.390</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.515</td><td align="center" valign="middle" >0.359</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x112.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.85</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.827</td><td align="center" valign="middle" >0.421</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.577</td><td align="center" valign="middle" >0.437</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x113.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.171</td><td align="center" valign="middle" >0.141</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.281</td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >16</td></tr></tbody></table></table-wrap><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Comparison of result of proposed method (PM) with Thaukral (TM) method</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Functions</th><th align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x114.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  >n</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >Run time</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >NFE</th></tr></thead><tr><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >TM</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >TM</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >TM</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x115.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.141</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x116.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.390</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.421</td><td align="center" valign="middle" >0.281</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x117.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.187</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" >0.140</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >16</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x118.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.265</td><td align="center" valign="middle" >0.109</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x119.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.406</td><td align="center" valign="middle" >0.374</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.484</td><td align="center" valign="middle" >0.484</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >24</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x120.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >122</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.655</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >488</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x121.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.234</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >0.219</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >8</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x122.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >28</td></tr><tr><td align="center" valign="middle" >4.5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.218</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >48</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x123.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.296</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x124.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.468</td><td align="center" valign="middle" >0.560</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.515</td><td align="center" valign="middle" >0.421</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x125.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.85</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.827</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.577</td><td align="center" valign="middle" >0.375</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x126.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.171</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.281</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >28</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Comparison of result of proposed method (PM) with Mir (MM) method</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >Functions</th><th align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x127.png" xlink:type="simple"/></inline-formula></th><th align="center" valign="middle"  colspan="2"  >n</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >Run time</th><th align="center" valign="middle" ></th><th align="center" valign="middle"  colspan="2"  >NFE</th></tr></thead><tr><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >MM</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >MM</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >PM</td><td align="center" valign="middle" >MM</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x128.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.140</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x129.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.390</td><td align="center" valign="middle" >0.297</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.421</td><td align="center" valign="middle" >0.218</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x130.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.5</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.187</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >55</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" >0.109</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x131.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.265</td><td align="center" valign="middle" >0.094</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x132.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.25</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.406</td><td align="center" valign="middle" >0.437</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.484</td><td align="center" valign="middle" >0.437</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >20</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x133.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1.5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.188</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x134.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.234</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.249</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x135.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3.5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" >0.125</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >25</td></tr><tr><td align="center" valign="middle" >4.5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.156</td><td align="center" valign="middle" >0.203</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >35</td><td align="center" valign="middle" >40</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x136.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >1</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.296</td><td align="center" valign="middle" >0.109</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x137.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.468</td><td align="center" valign="middle" >0.296</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle" >1.2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" >2</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.515</td><td align="center" valign="middle" >0.484</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >10</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x138.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >−0.85</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.827</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >50</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >DIV</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.577</td><td align="center" valign="middle" >-</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >-</td></tr><tr><td align="center" valign="middle"  rowspan="2"  ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x139.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.8</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.171</td><td align="center" valign="middle" >0.218</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle" >0</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >0.281</td><td align="center" valign="middle" >0.172</td><td align="center" valign="middle" ></td><td align="center" valign="middle" >25</td><td align="center" valign="middle" >20</td></tr></tbody></table></table-wrap><p>iteration. In this paper, the stoping criterion is<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x140.png" xlink:type="simple"/></inline-formula>. the Run time and the Number of function evaluations (NFE) are also given in Tables 1-5. “DIV” in the tables implies that the corresponding method is diverges. Furthermore, a comparison of the rate of convergence of the proposed method and Kou-Li method [<xref ref-type="bibr" rid="scirp.64928-ref8">8</xref>] for function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x141.png" xlink:type="simple"/></inline-formula> at point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x142.png" xlink:type="simple"/></inline-formula> is shown in <xref ref-type="fig" rid="fig1">Figure 1</xref>. The comparison is clearly marked on <xref ref-type="fig" rid="fig1">Figure 1</xref>. It should be noted that, Numerical computations reported here have been carried out in the MAPLE 18 environment. The results show that the speed of convergence in all methods discussed in this article, are depends on proper selection of the initial point. For example, in <xref ref-type="table" rid="table1">Table 1</xref> for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x143.png" xlink:type="simple"/></inline-formula>, choose an initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x144.png" xlink:type="simple"/></inline-formula> is leading to the divergence of Kou et al. method, whereas the choose the initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x140.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x141.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x142.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x143.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x144.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x145.png" xlink:type="simple"/></inline-formula> in the same method is leading to the coverage to the simple root a, see <xref ref-type="table" rid="table1">Table 1</xref>. In all examples, it is evident that the proposed approach, for any initial point is coverage to simple root of a.</p><p>The test functions are listed as follows:</p><disp-formula id="scirp.64928-formula455"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x146.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula456"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x147.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula457"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x148.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula458"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x149.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula459"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x150.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula460"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x151.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula461"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x152.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula462"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x153.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula463"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x154.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula464"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x155.png"  xlink:type="simple"/></disp-formula><fig-group id="fig1"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> A comparison of the rate of convergence of the proposed method and Kou et al. method for function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x157.png" xlink:type="simple"/></inline-formula> at point<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x158.png" xlink:type="simple"/></inline-formula>. The proposed and Kou et al. methods converged to the simple root <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x157.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x158.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x159.png" xlink:type="simple"/></inline-formula> in 3 and 433 iteration, respectively. This show that the PM method is vary faster with respect to the Kou et al. method. More details are given in <xref ref-type="table" rid="table1">Table 1</xref>.</title></caption><fig id ="fig1_1"><label></label><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/3-7403060x156.png"/></fig></fig-group><disp-formula id="scirp.64928-formula465"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x160.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64928-formula466"><graphic  xlink:href="http://html.scirp.org/file/3-7403060x161.png"  xlink:type="simple"/></disp-formula><p>One can easily see from Tables 1-5 that our method behaves either similarly or better then the compared methods. The results show that the new method has advantages over the Kou et al. [<xref ref-type="bibr" rid="scirp.64928-ref8">8</xref>] method and the eight-order method as Thukral [<xref ref-type="bibr" rid="scirp.64928-ref4">4</xref>] method. Also, the new method have iteration stabilities to the original iteration value and behave either similarly or better than the methods compared. All numerical results are in accordance with the theory and the basic advantage of the variants of Newton’s method based on means or integration methods that they do not require the computation of second- or higher-order derivatives although they are of ninth order.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In numerical analysis, many methods produce sequences of real numbers, for example the iterative schemes for solving<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x162.png" xlink:type="simple"/></inline-formula>. Sometimes, the convergence of these sequences is slow and their utility in solving practical problems, quite limited. Convergence acceleration methods try to transform a slowly converging sequence into a fast convergent one. Accordingly in this work, a new method has developed. In this study, a new ninth-order method to solve nonlinear equations has been proposed. From numerical examples, it has been observed that the proposed method convergence quickly toward root a is compared to lower order methods. In addition, in practical terms, the method is noticeable. Also, the above-mentioned ninth-order method requires the evaluation of three functions and two first derivatives of the function. Therefore, the new method has the efficiency index<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x163.png" xlink:type="simple"/></inline-formula>. Unlike the other methods, the proposed method converges well when the initial point <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x162.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x163.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/3-7403060x164.png" xlink:type="simple"/></inline-formula> is at the boot sides of root a. This is obviously clear understood from the examples.</p></sec><sec id="s6"><title>Cite this paper</title><p>ArminGhane-Kanafi,SohrabKordrostami, (2016) A New Approach for Solving Nonlinear Equations by Using of Integer Nonlinear Programming. Applied Mathematics,07,473-481. doi: 10.4236/am.2016.76043</p></sec><sec id="s7"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.64928-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Neta, B. (1979) A Sixth-Order Family of Methods for Nonlinear Equations. International Journal of Computer Mathematics, 7, 157-161. http://dx.doi.org/10.1080/00207167908803166</mixed-citation></ref><ref id="scirp.64928-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Parhi, S.K. and Gupta, D.K. (2008) A Sixth Order Method for Nonlinear Equations. Applied Mathematics and Computation, 203, 50-55. http://dx.doi.org/10.1016/j.amc.2008.03.037</mixed-citation></ref><ref id="scirp.64928-ref3"><label>3</label><mixed-citation publication-type="other" xlink:type="simple">Mir, N.A., Rafiq, N. and Akram, S. (2009) An Efficient Three-Step Iterative Method for Non-Linear Equations. 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