<?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.2014.27064</article-id><article-id pub-id-type="publisher-id">JAMP-46815</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>Steffensen-Type Method of Super Third-Order Convergence for Solving Nonlinear Equations</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Zhongli</surname><given-names>Liu</given-names></name></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hong</surname><given-names>Zhang</given-names></name></contrib></contrib-group><pub-date pub-type="epub"><day>13</day><month>06</month><year>2014</year></pub-date><volume>02</volume><issue>07</issue><fpage>581</fpage><lpage>586</lpage><history><date date-type="received"><day>5</day>	<month>March</month>	<year>2014</year></date><date date-type="rev-recd"><day>5</day>	<month>April</month>	<year>2014</year>	</date><date date-type="accepted"><day>12</day>	<month>April</month>	<year>2014</year></date></history><permissions><copyright-statement>&#169; Copyright  2014 by authors and Scientific Research Publishing Inc. </copyright-statement><copyright-year>2014</copyright-year><license><license-p>This work is licensed under the Creative Commons Attribution International License (CC BY). http://creativecommons.org/licenses/by/4.0/</license-p></license></permissions><abstract><p>
	In this paper, a
one-step Steffensen-type method with super-cubic convergence for solving nonlinear
equations is suggested. The convergence order 3.383 is proved theoretically and
demonstrated numerically. This super-cubic convergence is obtained by
self-accelerating second-order Steffensen’s method twice with memory, but
without any new function evaluations. The proposed method is very efficient and
convenient, since it is still a derivative-free two-point method. Its theoretical
results and high computational efficiency is confirmed by Numerical examples. 
</p></abstract><kwd-group><kwd>Newton’s Method</kwd><kwd> Steffensen’s Method</kwd><kwd> Derivative Free</kwd><kwd> Super-Cubic Convergence</kwd><kwd> Nonlinear Equation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Finding the root of a nonlinear equation</p><disp-formula id="scirp.46815-formula1"><label>(1)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\eabbe28a-f3eb-4481-a8c9-f1e664da14e1.png"/></disp-formula><p>is a classical problem. It is well-known in scientific computation that Newton’s method (NM, see [<xref ref-type="bibr" rid="scirp.46815-ref1">1</xref>] ):</p><disp-formula id="scirp.46815-formula2"><label>(2)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\9f9cd4fb-030e-4dfe-b373-be4b3c6a473c.png"/></disp-formula><p>is widely used for root-finding, where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\697e107a-f0b7-41bc-b1ae-4d531953a8cf.png" xlink:type="simple"/></inline-formula> is an initial guess of the root. However, when the derivative <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\e4c9ae5b-82df-4344-be6a-064f59c2ff6d.png" xlink:type="simple"/></inline-formula> is unavailable or is expensive to be obtained, the derivative-free method is necessary. If the derivative <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\73b40ed3-dc8e-4a92-baf3-5700868523a3.png" xlink:type="simple"/></inline-formula> is replaced by the divided difference in (2), Steffensen’s method (SM, see [<xref ref-type="bibr" rid="scirp.46815-ref1">1</xref>] ) is obtained as follows:</p><disp-formula id="scirp.46815-formula3"><label>(3)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\4787dfd0-0842-42a8-a3b7-0e0ed1b6cbc1.png"/></disp-formula><p>NM/SM converges quadratically and requires two function evaluations per iteration. The efficiency index of them is<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\de2bb038-555c-49e6-b7dd-e4cb92afa9e8.png" xlink:type="simple"/></inline-formula>.</p><p>Besides H.T. Kung and J.F. Traub conjectured that an iterative method based on <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\204c7c38-43d2-4355-b240-536edaef7c46.png" xlink:type="simple"/></inline-formula> evaluations per iteration without memory would arrive at the optimal convergence of order <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\8e57798f-5c8e-40e1-8372-7306364cd9b0.png" xlink:type="simple"/></inline-formula> (see [<xref ref-type="bibr" rid="scirp.46815-ref2">2</xref>] ), Traub proposed a self-acce- lerating two-point method of order 2.414 with memory (see [<xref ref-type="bibr" rid="scirp.46815-ref3">3</xref>] ):</p><disp-formula id="scirp.46815-formula4"><label>(4)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\509b6765-ecfb-4558-9f9a-9071095b439d.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\1aa34965-e458-4361-a82a-dab3b7b32299.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\ff5410d4-205d-45c0-9240-b4412bdd3f26.png" xlink:type="simple"/></inline-formula> or<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\66942ecc-f1fd-44af-b9df-e4a9925de4fb.png" xlink:type="simple"/></inline-formula>, etc.</p><p>A lot of self-accelerating Steffensen-type methods were derived in the literature (see [<xref ref-type="bibr" rid="scirp.46815-ref1">1</xref>] -[<xref ref-type="bibr" rid="scirp.46815-ref7">7</xref>] ). Steffensen-type methods and their applications in the solution of nonlinear systems and nonlinear differential equations were discussed in [<xref ref-type="bibr" rid="scirp.46815-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.46815-ref4">4</xref>] [<xref ref-type="bibr" rid="scirp.46815-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.46815-ref8">8</xref>] . Recently, by a new self-accelerating technique based on the second-order Newtonian</p><p>interpolatory polynomial<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\5b246255-a5ec-40a2-9f72-27d144a3012a.png" xlink:type="simple"/></inline-formula>, J. Džunića</p><p>and M.S. Petkovića proposed a cubically convergent Steffensen-like method (see [<xref ref-type="bibr" rid="scirp.46815-ref7">7</xref>] ):</p><disp-formula id="scirp.46815-formula5"><label>(5)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\2e78d26b-9b61-4450-a53d-5fb6eccaf615.png"/></disp-formula><p>In this study, a one-step Steffensen-type method is proposed by doubly-self-accelerating in Section 2, its super-cubic convergence is proved in Section 3, and numerical examples are demonstrated in Section 4.</p></sec><sec id="s2"><title>2. The Method of Steﬀensen-Type</title><p>By the first-order Newtonian interpolatory polynomial <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\343cb3a4-3878-47ed-b0f9-f4747c67333a.png" xlink:type="simple"/></inline-formula> and</p><disp-formula id="scirp.46815-formula6"><label>,</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\f37f5e7e-e099-41d8-b676-3b2f424c12af.png"/></disp-formula><p>we have <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\7a092d7f-3ba6-43a8-be68-8d195af15ebf.png" xlink:type="simple"/></inline-formula></p><p>where</p><disp-formula id="scirp.46815-formula7"><label>.</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\28451e90-5e19-45ec-b859-8a83ab7347a3.png"/></disp-formula><p>So, with some <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\fd25161b-289e-4608-8980-43fb4a205afe.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.46815-formula8"><label>(6)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\180bd8b3-b055-47c4-a722-4c5086f39ccb.png"/></disp-formula><p>should be better than <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\b21fcbc0-a6e1-4a5f-aedc-febe5b530529.png" xlink:type="simple"/></inline-formula> to approximate<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\2d15ddf4-735c-47d4-b5d2-9cbf354c03b2.png" xlink:type="simple"/></inline-formula>.</p><p>Therefore, we suggest <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\f1d1c699-03b7-4aac-b20a-56d8624ec9e0.png" xlink:type="simple"/></inline-formula> i.e., a two-parameter Steffensen’s method:</p><disp-formula id="scirp.46815-formula9"><label>(7)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\5b253d51-4fe6-4af8-802b-12519548f442.png"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\e7226e82-e473-44e5-b6fb-88102a4ffbbf.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\f6f9b40a-0484-4211-ad8c-a00aae95a108.png" xlink:type="simple"/></inline-formula>and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\fc355ad9-0659-453d-885b-8f22c7e0066a.png" xlink:type="simple"/></inline-formula> are bounded constant sequences. The error equation of (7) is</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\98a7c0a4-6fd3-4f03-926d-7d24d2e62d7d.png" xlink:type="simple"/></inline-formula>. By defining <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\a10b3b56-556b-4183-bb93-40033fb10f43.png" xlink:type="simple"/></inline-formula> and</p><p><inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\7d7bd4af-4884-4fb5-a37b-7c3eae3c6e2a.png" xlink:type="simple"/></inline-formula>recursively as the iteration proceeds without any new evaluation to</p><p>vanish the asymptotic convergence constant, we establish a self-accelerating Steffensen’s method with super quadratic convergence as follows:</p><disp-formula id="scirp.46815-formula10"><label>(8)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\5826cfb3-77e7-4186-975e-c5973fdea57b.png"/></disp-formula><p>Furthermore, we propose a one-step Steffensen-type method with super cubic convergence by doubly-self- accelerating as follows:</p><disp-formula id="scirp.46815-formula11"><label>(9)</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\25b8970e-45af-427a-88ba-adbecb888afe.png"/></disp-formula></sec><sec id="s3"><title>3. Its Super Third-Order Convergence</title><p>Lemma 3.1 <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\a1b765a7-72a9-4ff2-91e7-5cc907b01cf5.png" xlink:type="simple"/></inline-formula> where <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\c03870de-4193-43d2-9f86-85336cb3a896.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\a0a55bfc-ed93-48c6-b678-fed05cb3fc43.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\860a0358-40b9-41ce-b095-9678cee8e5b5.png" xlink:type="simple"/></inline-formula></p><p>Proof. By Taylor formula, we have</p><disp-formula id="scirp.46815-formula12"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\b9144fdb-ca39-4990-ab36-6360b6feda59.png"/></disp-formula><p>So,</p><disp-formula id="scirp.46815-formula13"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\c1642c73-3776-4e3f-8278-12d1de52d2bf.png"/></disp-formula><p>Then, the proof can be completed.</p><p>Theorem 3.2 Let <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6c459c5f-e7cd-44bf-9c7f-9d34cf5be5aa.png" xlink:type="simple"/></inline-formula> be a sufficiently differentiable function with simple root<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\931554a4-ad40-4909-89b7-5ddde387981e.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\f1a7ab03-4e4b-447e-90d5-e264ca511175.png" xlink:type="simple"/></inline-formula>be an open set, <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\9093bddf-5dc4-45d3-abff-e1dd71c9fd76.png" xlink:type="simple"/></inline-formula>be close enough to<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\0c5e910c-fa6c-4dd7-8e8c-ef39a916feac.png" xlink:type="simple"/></inline-formula>, then (9) achieve the convergence of order 3.383.</p><p>Proof. If <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\0274bc3c-d344-4ca4-b133-77a3472b01a7.png" xlink:type="simple"/></inline-formula> converges to <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\c2ca418f-6a92-4b53-baf7-bbd7df2bf920.png" xlink:type="simple"/></inline-formula> with order <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\722e5304-fc17-4f44-b59a-5ecbea01d2fe.png" xlink:type="simple"/></inline-formula> as:</p><disp-formula id="scirp.46815-formula14"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\21da937d-6c3f-40bc-ab12-71c2f3a4266d.png"/></disp-formula><p>and if <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\fd1b7e4b-6bda-4997-b7c4-b28df5e6e269.png" xlink:type="simple"/></inline-formula> converges to <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\ec58d401-865d-43df-ac0a-98c8c4d78d73.png" xlink:type="simple"/></inline-formula> with order <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\be10a0af-17f9-4582-9384-6e9d27b22394.png" xlink:type="simple"/></inline-formula> as:</p><disp-formula id="scirp.46815-formula15"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\e14477c8-90b2-471a-b7e9-bb3554980e30.png"/></disp-formula><p>Then</p><disp-formula id="scirp.46815-formula16"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\b9b26801-c35d-4630-90dd-ff69a35a6ac5.png"/></disp-formula><disp-formula id="scirp.46815-formula17"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\b9b26801-c35d-4630-90dd-ff69a35a6ac5.png"/></disp-formula><p>By Taylor formula and Lemma 3.1, we also have</p><disp-formula id="scirp.46815-formula18"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\400f2f2e-c3d0-438d-ab28-20c6783eadef.png"/></disp-formula><disp-formula id="scirp.46815-formula19"><label>.</label><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\ceeaea9a-b4e0-4aa2-90cc-c8fbcbf64ecf.png"/></disp-formula><p>So, comparing the exponents of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\5e674b09-660d-4b15-a3de-b05990e3d0f1.png" xlink:type="simple"/></inline-formula> in expressions of <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\4fe67c42-2c53-42fd-ad1c-c5b663b15b71.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\9402a72f-17a6-411a-a047-9df1b6b7fd1d.png" xlink:type="simple"/></inline-formula> for (9), we obtain the same system of two equations:</p><disp-formula id="scirp.46815-formula20"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\2d71e303-8607-48a1-ba96-442a11eff6bb.png"/></disp-formula><p>From its non-trivial solution <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\c811c12a-f7d2-4352-923c-dfe27a7ddb4b.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\c3eba652-c0fb-467c-a82a-097ef6e8d77a.png" xlink:type="simple"/></inline-formula>, we prove that the convergence of (9) is of order 3.383.</p><p>As the efficiency index is<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\bdf50c99-78d8-4225-91eb-f3c00245e62e.png" xlink:type="simple"/></inline-formula>, without any additional function evaluations, the efficiency indices of (4), (5)</p><p>and (9) are <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\a977cb85-e501-4dd1-8c7c-50e04c571da9.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\0928162e-4b89-4874-9486-18a6c0714562.png" xlink:type="simple"/></inline-formula> respectively.</p></sec><sec id="s4"><title>4. Numerical Examples</title><p>Related one-step methods only using two function evaluations per iteration are showed in the following numeri- cal examples. The proposed method is a derivative-free two-point method with high computational efficiency.</p><p>Example 1. The numerical results of NM, SM, (4), (5) and (9) in <xref ref-type="table" rid="table1">Table 1</xref> agree with the theoretical analysis. The computational order of convergence is defined by</p><disp-formula id="scirp.46815-formula21"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\0573e26d-3a80-4a7d-a4ea-b84d87f21900.png"/></disp-formula><p>Example 2. The numerical results of NM, SM, (4), (5) and (9) are in <xref ref-type="table" rid="table2">Table 2</xref> for the following nonlinear functions:</p><disp-formula id="scirp.46815-formula22"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\2a46a253-b53a-4d01-9624-e1e1c600d1a0.png"/></disp-formula><disp-formula id="scirp.46815-formula23"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\2a46a253-b53a-4d01-9624-e1e1c600d1a0.png"/></disp-formula><disp-formula id="scirp.46815-formula24"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\2a46a253-b53a-4d01-9624-e1e1c600d1a0.png"/></disp-formula><disp-formula id="scirp.46815-formula25"><inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\2a46a253-b53a-4d01-9624-e1e1c600d1a0.png"/></disp-formula><p><xref ref-type="table" rid="table1">Table 1</xref>.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</p><table-wrap id="table1"  position="float"><object-id pub-id-type="pii">Table 1</object-id><label>Table 1</label><caption><p>.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</p></caption><table><thead><tr><th align="center" valign="middle" >Methods</th><th align="center" valign="middle" >n</th><th align="center" valign="middle" >1</th><th align="center" valign="middle" >2</th><th align="center" valign="middle" >3</th><th align="center" valign="middle" >4</th><th align="center" valign="middle" >5</th><th align="center" valign="middle" >6</th></tr></thead><tbody><tr><td align="center" valign="middle" >NM</td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >0.53279e−2</td><td align="center" valign="middle" >0.35561e−5</td><td align="center" valign="middle" >0.15808e−11</td><td align="center" valign="middle" >0.31235e−24</td><td align="center" valign="middle" >0.12195e−49</td><td align="center" valign="middle" >0.15890e−100</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >2.25256</td><td align="center" valign="middle" >2.01691</td><td align="center" valign="middle" >0.15808e−11</td><td align="center" valign="middle" >2.00000</td><td align="center" valign="middle" >2.00000</td><td align="center" valign="middle" >2.00000</td></tr><tr><td align="center" valign="middle" >SM</td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >0.28174e−1</td><td align="center" valign="middle" >0.51325e−3</td><td align="center" valign="middle" >0.16476e−6</td><td align="center" valign="middle" >0.16966e−13</td><td align="center" valign="middle" >0.17989e−27</td><td align="center" valign="middle" >0.20226e−55</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >1.21776</td><td align="center" valign="middle" >2.04376</td><td align="center" valign="middle" >2.00830</td><td align="center" valign="middle" >2.00009</td><td align="center" valign="middle" >2.00000</td><td align="center" valign="middle" >2.00000</td></tr><tr><td align="center" valign="middle" >(4)</td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >0.28174e−1</td><td align="center" valign="middle" >0.15996e−4</td><td align="center" valign="middle" >0.13132e−12</td><td align="center" valign="middle" >0.43283e−32</td><td align="center" valign="middle" >0.38442e−79</td><td align="center" valign="middle" >0.99936−193</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >1.21776</td><td align="center" valign="middle" >3.81335</td><td align="center" valign="middle" >2.49109</td><td align="center" valign="middle" >2.40945</td><td align="center" valign="middle" >2.41512</td><td align="center" valign="middle" >2.41406</td></tr><tr><td align="center" valign="middle" >(5)</td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >0.28174e−1</td><td align="center" valign="middle" >0.16560e−6</td><td align="center" valign="middle" >0.11521e−21</td><td align="center" valign="middle" >0.39821e−67</td><td align="center" valign="middle" >0.16444e−203</td><td align="center" valign="middle" >0.11580e−612</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >1.21776</td><td align="center" valign="middle" >6.14536</td><td align="center" valign="middle" >2.89776</td><td align="center" valign="middle" >2.99925</td><td align="center" valign="middle" >3.00000</td><td align="center" valign="middle" >3.00000</td></tr><tr><td align="center" valign="middle" >(9)</td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >0.28174e−1</td><td align="center" valign="middle" >0.43010e−7</td><td align="center" valign="middle" >0.21604e−27</td><td align="center" valign="middle" >0.23153e−94</td><td align="center" valign="middle" >0.20021e−321</td><td align="center" valign="middle" >0.69689e−1090</td></tr><tr><td align="center" valign="middle" ></td><td align="center" valign="middle" >.<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\6d982112-bfb6-461f-99b8-09afc536bade.png" xlink:type="simple"/></inline-formula>.</td><td align="center" valign="middle" >1.21776</td><td align="center" valign="middle" >6.83322</td><td align="center" valign="middle" >3.49004</td><td align="center" valign="middle" >3.29917</td><td align="center" valign="middle" >3.39052</td><td align="center" valign="middle" >3.38434</td></tr></tbody></table></table-wrap><p><xref ref-type="table" rid="table2">Table 2</xref>. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></p><table-wrap id="table2"  position="float"><object-id pub-id-type="pii">Table 2</object-id><label>Table 2</label><caption><p>. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></p></caption><table><thead><tr><th align="center" valign="middle" >Methods</th><th align="center" valign="middle" >NM</th><th align="center" valign="middle" >SM</th><th align="center" valign="middle" >(4)</th><th align="center" valign="middle" >(5)</th><th align="center" valign="middle" >(9)</th></tr></thead><tbody><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.19785e−40</td><td align="center" valign="middle" >0.88156e−29</td><td align="center" valign="middle" >0.50439e−84</td><td align="center" valign="middle" >0.19314e−313</td><td align="center" valign="middle" >0.75162e−578</td></tr><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.4141</td><td align="center" valign="middle" >3.0000</td><td align="center" valign="middle" >3.3831</td></tr><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.32328e−44</td><td align="center" valign="middle" >0.42920e−26</td><td align="center" valign="middle" >0.19843e−85</td><td align="center" valign="middle" >0.57587e−282</td><td align="center" valign="middle" >0.13494e−706</td></tr><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.4141</td><td align="center" valign="middle" >3.0000</td><td align="center" valign="middle" >3.3825</td></tr><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.18813e−51</td><td align="center" valign="middle" >0.15758e−18</td><td align="center" valign="middle" >0.12013e−86</td><td align="center" valign="middle" >0.34524e−286</td><td align="center" valign="middle" >0.27679e−677</td></tr><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.4140</td><td align="center" valign="middle" >3.0000</td><td align="center" valign="middle" >3.3796</td></tr><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >0.35988e−79</td><td align="center" valign="middle" >0.96290e−84</td><td align="center" valign="middle" >0.16834e−248</td><td align="center" valign="middle" >0.21536e−597</td><td align="center" valign="middle" >0.25291e−1154</td></tr><tr><td align="center" valign="middle" >. Numerical results for solving<inline-formula><inline-graphic xlink:href="http://file.scirp.org/Html/htmlimages\10-1720121x\59324de1-7c54-4906-978a-7ef726f0922e.png" xlink:type="simple"/></inline-formula></td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.0000</td><td align="center" valign="middle" >2.4161</td><td align="center" valign="middle" >3.0000</td><td align="center" valign="middle" >3.3831</td></tr></tbody></table></table-wrap></sec><sec id="s5"><title>5. Conclusion</title><p>By theoretical analysis and numerical experiments, we confirm that the proposed method which is a derivative- free two-point method has high computational efficiency. Its convergence order is 3.383 and its efficiency index is 1.839. 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