<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2016.43058</article-id><article-id pub-id-type="publisher-id">JAMP-64904</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  New Fourth Order Iterative Methods Second Derivative Free
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>sama</surname><given-names>Y. Ababneh</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Zarqa University, Zarqa, Jordan</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>osababneh@zu.edu.jo</email></corresp></author-notes><pub-date pub-type="epub"><day>21</day><month>03</month><year>2016</year></pub-date><volume>04</volume><issue>03</issue><fpage>519</fpage><lpage>523</lpage><history><date date-type="received"><day>23</day>	<month>February</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>20</month>	<year>March</year>	</date><date date-type="accepted"><day>23</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>
 
 
  In a recent paper, Noor and Khan [M. Aslam Noor, &amp; W. A. Khan, (2012) New Iterative Methods for Solving Nonlinear Equation by Using Homotopy Perturbation Method, Applied Mathematics and Computation, 219, 3565-3574], suggested a fourth-order method for solving nonlinear equations. Per iteration in this method requires two evaluations of the function and two of its first derivatives; therefore, the efficiency index is 1.41421 as Newton’s method. In this paper, we modified this method and obtained a family of iterative methods for appropriate and suitable choice of the parameter. It should be noted that per iteration for the new methods requires two evaluations of the function and one evaluation of its first derivatives, so its efficiency index equals to 1.5874. Analysis of convergence shows that the methods are fourth-order. Several numerical examples are given to illustrate the performance of the presented methods.
 
</p></abstract><kwd-group><kwd>Newton’s Method</kwd><kwd> Fourth-Order Convergence</kwd><kwd> Third-Order Convergence</kwd><kwd> Non-Linear Equations</kwd><kwd> Root-Finding</kwd><kwd> Iterative Method</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In this paper, we consider iterative methods to find a simple root of a nonlinear equation f(x) = 0, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x6.png" xlink:type="simple"/></inline-formula> for an open interval D is a scalar function. The classical Newton’s method is given by</p><disp-formula id="scirp.64904-formula517"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x7.png"  xlink:type="simple"/></disp-formula><p>This is an important and basic method [<xref ref-type="bibr" rid="scirp.64904-ref1">1</xref>] , which converges quadratically. Recently, Noor [<xref ref-type="bibr" rid="scirp.64904-ref2">2</xref>] proposed a new fourth-order method defined by</p><disp-formula id="scirp.64904-formula518"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x8.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x9.png" xlink:type="simple"/></inline-formula></p><p>It is clear that to implement (2), one has to evaluate the second derivative of the function. This can create some problems. In order to overcome this drawback, several techniques have been developed [<xref ref-type="bibr" rid="scirp.64904-ref3">3</xref>] - [<xref ref-type="bibr" rid="scirp.64904-ref6">6</xref>] . In [<xref ref-type="bibr" rid="scirp.64904-ref7">7</xref>] , a second-derivative-free method is obtained through approximating the second derivative <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x10.png" xlink:type="simple"/></inline-formula> in (3) by</p><disp-formula id="scirp.64904-formula519"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x11.png"  xlink:type="simple"/></disp-formula><p>In a recent paper, Noor and Khan [<xref ref-type="bibr" rid="scirp.64904-ref8">8</xref>] have used the same approximation of the second derivative (3) in (2) to suggest the following Iterative methods</p><disp-formula id="scirp.64904-formula520"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x12.png"  xlink:type="simple"/></disp-formula><p>In this paper, we rederive the method in (4) to obtain a family of fourth-order method free from second derivative. Moreover, per iteration in these new methods requires two evaluations of the function and just one of its first derivatives.</p><p>The rest of this paper is organized as follows. The proposed methods are described in Section 2. In Section 3, the convergence analysis is carried out to establish the order of convergence. Finally, in Section 4, the methods are tested on some numerical examples and comparisons of the results of our methods.</p></sec><sec id="s2"><title>2. Description of the Methods</title><p>The following approximations of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x13.png" xlink:type="simple"/></inline-formula> are obtained in [<xref ref-type="bibr" rid="scirp.64904-ref9">9</xref>]</p><disp-formula id="scirp.64904-formula521"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x14.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.64904-formula522"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x15.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x16.png" xlink:type="simple"/></inline-formula>. We then apply the approximations (5) and (6) to the method (4). Now, Combining (5) and (4), we get the new iterative method</p><disp-formula id="scirp.64904-formula523"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x17.png"  xlink:type="simple"/></disp-formula><p>Using (6) in (4), we get a new family of iterative method</p><disp-formula id="scirp.64904-formula524"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x18.png"  xlink:type="simple"/></disp-formula><p>Essentially, we consider the convergence criteria of the new methods in (7) and (8), and this is the main motivation of our next result.</p></sec><sec id="s3"><title>3. The Analysis of Convergence</title><p>Theorem 1. Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x19.png" xlink:type="simple"/></inline-formula> be a simple zero of sufficiently differentiable function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x20.png" xlink:type="simple"/></inline-formula> for an open interval I. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x21.png" xlink:type="simple"/></inline-formula> is sufficiently close to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x22.png" xlink:type="simple"/></inline-formula>, where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x23.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x20.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x23.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x24.png" xlink:type="simple"/></inline-formula>. Then the methods defined by (7) and (8) are of fourth-order convergence and satisfy the error equations</p><disp-formula id="scirp.64904-formula525"><graphic  xlink:href="http://html.scirp.org/file/4-1720532x25.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.64904-formula526"><graphic  xlink:href="http://html.scirp.org/file/4-1720532x26.png"  xlink:type="simple"/></disp-formula><p>Proof.</p><p>Using Taylor expansion of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x27.png" xlink:type="simple"/></inline-formula> about <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x28.png" xlink:type="simple"/></inline-formula> and taking into account that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x28.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x29.png" xlink:type="simple"/></inline-formula>, we have</p><disp-formula id="scirp.64904-formula527"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x30.png"  xlink:type="simple"/></disp-formula><p>Furthermore, we have</p><disp-formula id="scirp.64904-formula528"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x31.png"  xlink:type="simple"/></disp-formula><p>and</p><disp-formula id="scirp.64904-formula529"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x32.png"  xlink:type="simple"/></disp-formula><p>Substituting (11) in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x33.png" xlink:type="simple"/></inline-formula> yields</p><disp-formula id="scirp.64904-formula530"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x34.png"  xlink:type="simple"/></disp-formula><p>Expanding <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x35.png" xlink:type="simple"/></inline-formula> about α and using (12), we have</p><disp-formula id="scirp.64904-formula531"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x36.png"  xlink:type="simple"/></disp-formula><p>Using Equations (9)-(13) in method (7) we have the following error equation:</p><disp-formula id="scirp.64904-formula532"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x37.png"  xlink:type="simple"/></disp-formula><p>this means that the method defined by (7) is fourth order. Also, using Equations (9)-(13) in (8) we get the following error equation:</p><disp-formula id="scirp.64904-formula533"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/4-1720532x38.png"  xlink:type="simple"/></disp-formula><p>which means that the family defined by (8) is of order four<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x39.png" xlink:type="simple"/></inline-formula>.</p><p>This completes the proof of the theorem.</p><p>If we consider the definition of efficiency index as<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x40.png" xlink:type="simple"/></inline-formula>, where p is the order of the method and w is the</p><p>number of function evaluations per iteration required by the method, then the fourth-order method (4) has the efficiency index equal to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x41.png" xlink:type="simple"/></inline-formula>, while for the newfourth order methods (7) and (8) is <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x41.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x42.png" xlink:type="simple"/></inline-formula> which is better than method defined by (4).</p></sec><sec id="s4"><title>4. Numerical Results</title><p>All computations were done using the Mathematica package using 64 digit floating point arithmetic’s. We accept an approximate solution rather than the exact root, depending on the precision (ϵ) of the computer. We use the following stopping criteria for computer programs: <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x43.png" xlink:type="simple"/></inline-formula>and so, when the stopping criterion is satisfied, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x44.png" xlink:type="simple"/></inline-formula>is taken as the exact root α computed. We used the fixed stopping criterion<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x43.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x45.png" xlink:type="simple"/></inline-formula>.</p><p>It is well-known that the convergence of iteration formula is guaranteed only when the initial approximation is sufficiently near to root. In general, it may be divergent when initial approximation is far from the root.</p><p>We employ the present methods to solve some nonlinear equations, which not only illustrate the methods practically but also serve to check the validity of theoretical results we have derived, the following</p><disp-formula id="scirp.64904-formula534"><graphic  xlink:href="http://html.scirp.org/file/4-1720532x46.png"  xlink:type="simple"/></disp-formula><p>Displayed in <xref ref-type="table" rid="table1">Table 1</xref> the number of iterations to approximate the zero (N) and the number of function evaluations (TNFE) counted as the sum of the number of evaluations of the function itself plus the number of evaluations of the derivative. We present some numerical test results for various iterative schemes in <xref ref-type="table" rid="table1">Table 1</xref>.</p><p>Compared with the Newton method (NM), the method in (4) (NOR), the new methods in (7) (MNR1), and as an example of (8) we take β = 0 (MNR2), and β = 1 (MNR3). The test results in <xref ref-type="table" rid="table1">Table 1</xref> show that for most of the functions we tested. Note that we used NC in <xref ref-type="table" rid="table1">Table 1</xref> to mean that the method does not converge to the root. The new methods introduced in the present presentation have at least equal performance compared to the method in (4), and better than Newton method. As far as the results we consider, the new fourth-order methods, require the less NFEs as compared to the Newton’s method and method in (4).</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Comparison of various fourth order schemes and Newton’s method</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  ></th><th align="center" valign="middle"  colspan="5"  >N</th><th align="center" valign="middle"  colspan="5"  >TNFE</th></tr></thead><tr><td align="center" valign="middle" >NM</td><td align="center" valign="middle" >NOR</td><td align="center" valign="middle" >MNR1</td><td align="center" valign="middle" >MNR2</td><td align="center" valign="middle" >MNR3</td><td align="center" valign="middle" >NM</td><td align="center" valign="middle" >NOR</td><td align="center" valign="middle" >MNR1</td><td align="center" valign="middle" >MNR2</td><td align="center" valign="middle" >MNR3</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x47.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >5</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" >3</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x48.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >53</td><td align="center" valign="middle" >38</td><td align="center" valign="middle" >22</td><td align="center" valign="middle" >56</td><td align="center" valign="middle" >17</td><td align="center" valign="middle" >106</td><td align="center" valign="middle" >152</td><td align="center" valign="middle" >66</td><td align="center" valign="middle" >168</td><td align="center" valign="middle" >51</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x49.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x50.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x51.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >4</td><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" >2</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x52.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >5</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" >3</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x53.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >4</td><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" >2</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x54.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >4</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" >3</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x55.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >NC</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >3</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" >16</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >9</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x56.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >18</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >18</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x57.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >3</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >10</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >9</td><td align="center" valign="middle" >12</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x58.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x59.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >16</td><td align="center" valign="middle" >20</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >15</td><td align="center" valign="middle" >15</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x60.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >4</td><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" >2</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >8</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >6</td><td align="center" valign="middle" >6</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x61.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >24</td><td align="center" valign="middle" >28</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >21</td><td align="center" valign="middle" >21</td></tr><tr><td align="center" valign="middle" ><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/4-1720532x62.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >19</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >11</td><td align="center" valign="middle" >12</td><td align="center" valign="middle" >38</td><td align="center" valign="middle" >44</td><td align="center" valign="middle" >36</td><td align="center" valign="middle" >33</td><td align="center" valign="middle" >36</td></tr></tbody></table></table-wrap><p>As a conclusion, we can infer that the present method has better performance in accordance with the theoretical analysis of the order. However, it should be noted that per iteration the methods (MNR1), (MNR2) and (MNR32) do require two evaluations of the function and one of its first derivative, whereas the method (4) does require two evaluations of the function and two of its first derivative, costing more expensive computation. Thus, the present methods can be of practical interest.</p></sec><sec id="s5"><title>5. Conclusions</title><p>We have proposed new fourth order methods of iterative methods for solving nonlinear equations. Numerical results show that the number of iterations of the new method is always less than that of the classical Newton’s method and the method in (4).</p><p>Analysis of convergence of methods is supplied in Theorem 2. Analysis of efficiency shows that these methods are preferable to Newton’s method and the fourth order method in (4). The number of function evaluations of the new methods is comparable.</p></sec><sec id="s6"><title>Acknowledgements</title><p>This research is funded by the Deanship of Research in Zarqa University/Jordan.</p></sec><sec id="s7"><title>Cite this paper</title><p>Osama Y.Ababneh, (2016) New Fourth Order Iterative Methods Second Derivative Free. Journal of Applied Mathematics and Physics,04,519-523. doi: 10.4236/jamp.2016.43058</p></sec></body><back><ref-list><title>References</title><ref id="scirp.64904-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Ostrowski, A.M. (1973) Solution of Equations in Eucilidean and Banach Space. 3rd Edition, Academic Press, New York.</mixed-citation></ref><ref id="scirp.64904-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Noor, M.A. (2010) Some Iterative Methods for Solving Nonlinear Equations Using Homotopy Perturbation Method. 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