<?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.2016.711106</article-id><article-id pub-id-type="publisher-id">AM-68151</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 Remarkable Chord Iterative Method for Roots of Uncertain Multiplicity
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>I.</surname><given-names>Fried</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Boston University, Boston, MA, USA</addr-line></aff><author-notes><corresp id="cor1">* E-mail:</corresp></author-notes><pub-date pub-type="epub"><day>11</day><month>07</month><year>2016</year></pub-date><volume>07</volume><issue>11</issue><fpage>1207</fpage><lpage>1214</lpage><history><date date-type="received"><day>23</day>	<month>May</month>	<year>2016</year></date><date date-type="rev-recd"><day>accepted</day>	<month>8</month>	<year>July</year>	</date><date date-type="accepted"><day>11</day>	<month>July</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 this note we at first briefly review iterative methods for effectively approaching a root of an unknown multiplicity. We describe a first order, then a second order estimate for the multiplicity index m of the approached root. Next we present a second order, two-step method for iteratively nearing a root of an unknown multiplicity. Subsequently, we introduce a novel chord, or a two- step method, not requiring beforehand knowledge of the multiplicity index m of the sought root, nor requiring higher order derivatives of the equilibrium function, which is quadratically convergent for any , and then reverts to superlinear.
 
</p></abstract><kwd-group><kwd>Iterative Methods</kwd><kwd> Unknown Root Multiplicity</kwd><kwd> Two-Step Methods</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The multiplicity index m of root<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x7.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x8.png" xlink:type="simple"/></inline-formula>of equilibrium function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x9.png" xlink:type="simple"/></inline-formula> may be a well latent property of the root, not cursorily revealed, nor readily available, yet this multiplicity can profoundly affect the behavior of the iterative approach [<xref ref-type="bibr" rid="scirp.68151-ref1">1</xref>] - [<xref ref-type="bibr" rid="scirp.68151-ref3">3</xref>] to the root. In this note, we briefly review the iterative methods [<xref ref-type="bibr" rid="scirp.68151-ref4">4</xref>] - [<xref ref-type="bibr" rid="scirp.68151-ref8">8</xref>] for approaching a root of an unknown multiplicity, and present a first oder [<xref ref-type="bibr" rid="scirp.68151-ref9">9</xref>] as well as a second order estimate for the multiplicity index m of the approached root. Then we present a novel chord, or a two-step method, not requiring beforehand knowledge of m, nor requiring the higher derivatives of the equilibrium function, which is quadratically convergent for any<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x10.png" xlink:type="simple"/></inline-formula>, and then reverts to superlinear.</p></sec><sec id="s2"><title>2. Assumed Nature of the Equilibrium Function</title><p>We assume that near root<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x11.png" xlink:type="simple"/></inline-formula>, function <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x12.png" xlink:type="simple"/></inline-formula> has the power series representation</p><disp-formula id="scirp.68151-formula17"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x13.png"  xlink:type="simple"/></disp-formula><p>where m is the multiplicity index of root a, and where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x14.png" xlink:type="simple"/></inline-formula> etc. are, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x15.png" xlink:type="simple"/></inline-formula>, the coefficients</p><disp-formula id="scirp.68151-formula18"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x16.png"  xlink:type="simple"/></disp-formula><p>and so on.</p></sec><sec id="s3"><title>3. The Newton-Raphson Method</title><p>The Newton-Raphson method</p><disp-formula id="scirp.68151-formula19"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x17.png"  xlink:type="simple"/></disp-formula><p>is quadratic</p><disp-formula id="scirp.68151-formula20"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x18.png"  xlink:type="simple"/></disp-formula><p>if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x19.png" xlink:type="simple"/></inline-formula>. However, if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x20.png" xlink:type="simple"/></inline-formula>, the method declines to mere linear</p><disp-formula id="scirp.68151-formula21"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x21.png"  xlink:type="simple"/></disp-formula><p>See also [<xref ref-type="bibr" rid="scirp.68151-ref10">10</xref>] .</p></sec><sec id="s4"><title>4. Extrapolation to the Limit</title><p>Let <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x22.png" xlink:type="simple"/></inline-formula> be already near root a. Then, if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x23.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula22"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x24.png"  xlink:type="simple"/></disp-formula><p>nearly. Eliminating <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x25.png" xlink:type="simple"/></inline-formula> from the two equations we obtain</p><disp-formula id="scirp.68151-formula23"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x26.png"  xlink:type="simple"/></disp-formula><p>which we solve for an approximate a, as</p><disp-formula id="scirp.68151-formula24"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x27.png"  xlink:type="simple"/></disp-formula><p>where</p><disp-formula id="scirp.68151-formula25"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x28.png"  xlink:type="simple"/></disp-formula><p>The square root in Equation (8) may be approximated as</p><disp-formula id="scirp.68151-formula26"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x29.png"  xlink:type="simple"/></disp-formula><p>and for this extrapolated <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x30.png" xlink:type="simple"/></inline-formula> of Equation (8) we have</p><disp-formula id="scirp.68151-formula27"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x31.png"  xlink:type="simple"/></disp-formula><p>For example, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x32.png" xlink:type="simple"/></inline-formula>, and starting with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x33.png" xlink:type="simple"/></inline-formula>, we compute<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x34.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x35.png" xlink:type="simple"/></inline-formula>; and then from Equation (8),<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x36.png" xlink:type="simple"/></inline-formula>. Another such cycle starting with <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x37.png" xlink:type="simple"/></inline-formula> produces a next<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x32.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x33.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x34.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x35.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x36.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x37.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x38.png" xlink:type="simple"/></inline-formula>.</p></sec><sec id="s5"><title>5. Always Quadratic Newton-Raphson Method</title><p>The modified Newton-Raphson method</p><disp-formula id="scirp.68151-formula28"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x39.png"  xlink:type="simple"/></disp-formula><p>converges quadratically to a root of any multiplicity m</p><disp-formula id="scirp.68151-formula29"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x40.png"  xlink:type="simple"/></disp-formula><p>But for this we need to know m.</p><p>By Equation (1) we readily deduce that, for any x</p><disp-formula id="scirp.68151-formula30"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x41.png"  xlink:type="simple"/></disp-formula><p>obtained at the price of a second derivative. For finite-difference approximations of the needed derivatives see [<xref ref-type="bibr" rid="scirp.68151-ref11">11</xref>] - [<xref ref-type="bibr" rid="scirp.68151-ref13">13</xref>] . Using <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x42.png" xlink:type="simple"/></inline-formula> in Equation (14) for m in Equation (12) we obtain the method</p><disp-formula id="scirp.68151-formula31"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x43.png"  xlink:type="simple"/></disp-formula><p>which is quadratic for any, provided, m</p><disp-formula id="scirp.68151-formula32"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x44.png"  xlink:type="simple"/></disp-formula><p>The method of Equation (15) is also obtained by applying Newton’s method not to f, but rather to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x45.png" xlink:type="simple"/></inline-formula>. For<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x46.png" xlink:type="simple"/></inline-formula>, we obtain by the method of Equation (15) that requires not only <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x47.png" xlink:type="simple"/></inline-formula> but also<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x48.png" xlink:type="simple"/></inline-formula>, starting with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x46.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x47.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x49.png" xlink:type="simple"/></inline-formula>.</p><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x50.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula33"><label>(17a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x51.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x52.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula34"><label>(17b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x53.png"  xlink:type="simple"/></disp-formula><p>Equation (15) may be written as</p><disp-formula id="scirp.68151-formula35"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x54.png"  xlink:type="simple"/></disp-formula><p>and it is of interest to know that</p><disp-formula id="scirp.68151-formula36"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x55.png"  xlink:type="simple"/></disp-formula><p>For the price of a third derivative we may have the quadratic approximation</p><disp-formula id="scirp.68151-formula37"><label>(20)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x56.png"  xlink:type="simple"/></disp-formula></sec><sec id="s6"><title>6. An Erroneous m</title><p>The method</p><disp-formula id="scirp.68151-formula38"><label>(21)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x57.png"  xlink:type="simple"/></disp-formula><p>produces the superlinear</p><disp-formula id="scirp.68151-formula39"><label>(22)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x58.png"  xlink:type="simple"/></disp-formula><p>and if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x59.png" xlink:type="simple"/></inline-formula>, convergence is alternating.</p></sec><sec id="s7"><title>7. Estimation of the Leading Term</title><p>We readily have that</p><disp-formula id="scirp.68151-formula40"><label>(23)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x60.png"  xlink:type="simple"/></disp-formula><p>For example, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x61.png" xlink:type="simple"/></inline-formula>, we compute using Equation (23) the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x61.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x62.png" xlink:type="simple"/></inline-formula> approximations as depending on the chosen x</p><disp-formula id="scirp.68151-formula41"><label>(24)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x63.png"  xlink:type="simple"/></disp-formula></sec><sec id="s8"><title>8. An Elementary Discrete Two-Step Newton Method for Roots of Any Multiplicity</title><p>If</p><disp-formula id="scirp.68151-formula42"><label>(25)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x64.png"  xlink:type="simple"/></disp-formula><p>are already close to root a of multiplicity<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x65.png" xlink:type="simple"/></inline-formula>, then according to Equation (5)</p><disp-formula id="scirp.68151-formula43"><label>(26)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x66.png"  xlink:type="simple"/></disp-formula><p>nearly, from which we extract the approximation</p><disp-formula id="scirp.68151-formula44"><label>(27)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x67.png"  xlink:type="simple"/></disp-formula><p>Setting a back into Equation (26) yields</p><disp-formula id="scirp.68151-formula45"><label>(28)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x68.png"  xlink:type="simple"/></disp-formula><p>and the two-step method</p><disp-formula id="scirp.68151-formula46"><label>(29)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x69.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x70.png" xlink:type="simple"/></inline-formula> in Equation (28) is seen to be but the finite-difference approximation of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x70.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x71.png" xlink:type="simple"/></inline-formula> in Equation (14).</p><p>For example, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x72.png" xlink:type="simple"/></inline-formula>, and starting with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x72.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x73.png" xlink:type="simple"/></inline-formula>, we compute by Equation (29), the successive approximations</p><disp-formula id="scirp.68151-formula47"><label>(30a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x74.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68151-formula48"><label>(30b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x75.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68151-formula49"><label>(30c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x76.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.68151-formula50"><label>(30d)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x77.png"  xlink:type="simple"/></disp-formula><p>Generally, starting with</p><disp-formula id="scirp.68151-formula51"><label>(31)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x78.png"  xlink:type="simple"/></disp-formula><p>we have from the method of Equation (29) that</p><disp-formula id="scirp.68151-formula52"><label>(32)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x79.png"  xlink:type="simple"/></disp-formula><p>The repeated classical Newton’s method, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x80.png" xlink:type="simple"/></inline-formula>, we recall, is only linear if <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x80.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x81.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula53"><label>(33)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x82.png"  xlink:type="simple"/></disp-formula><p>See also [<xref ref-type="bibr" rid="scirp.68151-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.68151-ref15">15</xref>] .</p></sec><sec id="s9"><title>9. Derivation of the Chord Method</title><p>It is a rational two step method of the form</p><disp-formula id="scirp.68151-formula54"><label>(34)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x83.png"  xlink:type="simple"/></disp-formula><p>With</p><disp-formula id="scirp.68151-formula55"><label>(35)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x84.png"  xlink:type="simple"/></disp-formula><p>the method is quadratic for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x85.png" xlink:type="simple"/></inline-formula> and<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x85.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x86.png" xlink:type="simple"/></inline-formula>. In fact;</p><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x87.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula56"><label>(36a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x88.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x89.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula57"><label>(36b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x90.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x91.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula58"><label>(36c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x92.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x93.png" xlink:type="simple"/></inline-formula> the method produces</p><disp-formula id="scirp.68151-formula59"><label>(37)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x94.png"  xlink:type="simple"/></disp-formula><p>and for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x95.png" xlink:type="simple"/></inline-formula> the method is quadratic for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x95.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x96.png" xlink:type="simple"/></inline-formula> as well.</p><p>According to Equation (36a), if<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x97.png" xlink:type="simple"/></inline-formula>, then the method is higher than quadratic.</p></sec><sec id="s10"><title>10. The Method is Further Superlinear</title><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x98.png" xlink:type="simple"/></inline-formula> we have:</p><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x99.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula60"><label>(38a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x100.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x101.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula61"><label>(38b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x102.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x103.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula62"><label>(38c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x104.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x105.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula63"><label>(38d)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x106.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x107.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula64"><label>(38e)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x108.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x109.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula65"><label>(38f)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x110.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x111.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula66"><label>(38g)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x112.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x113.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula67"><label>(38h)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x114.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x115.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula68"><label>(38k)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x116.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x117.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula69"><label>(38l)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x118.png"  xlink:type="simple"/></disp-formula></sec><sec id="s11"><title>11. Lowering the Value of k</title><p>We leave k in <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x119.png" xlink:type="simple"/></inline-formula> of Equation (34), free, and have by power series expansion, for multiplicity index<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x120.png" xlink:type="simple"/></inline-formula>, for <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x119.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x120.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x121.png" xlink:type="simple"/></inline-formula> in Equation (1), that</p><disp-formula id="scirp.68151-formula70"><label>(39)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x122.png"  xlink:type="simple"/></disp-formula><p>The linear term in the above expansion is annulled with</p><disp-formula id="scirp.68151-formula71"><label>(40)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x123.png"  xlink:type="simple"/></disp-formula><p>We do this for higher values of m and find that</p><disp-formula id="scirp.68151-formula72"><label>(41)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x124.png"  xlink:type="simple"/></disp-formula><p>We try<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x125.png" xlink:type="simple"/></inline-formula>, and get</p><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x126.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula73"><label>(42a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x127.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x128.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula74"><label>(42b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x129.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x130.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula75"><label>(42c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x131.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x132.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula76"><label>(42d)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x133.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x134.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula77"><label>(42e)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x135.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x136.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula78"><label>(42f)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x137.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x138.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula79"><label>(42g)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x139.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x140.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula80"><label>(42h)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x141.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x142.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula81"><label>(42k)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x143.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x144.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula82"><label>(42l)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x145.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x146.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula83"><label>(42m)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x147.png"  xlink:type="simple"/></disp-formula><p>The general form of the linear part of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula> in Equations (42) is of the form <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x149.png" xlink:type="simple"/></inline-formula> with a constant <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x150.png" xlink:type="simple"/></inline-formula> that is small if multiplicity index m is not much above 5. For instance, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x151.png" xlink:type="simple"/></inline-formula>, meaning that at each iteration the error <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x152.png" xlink:type="simple"/></inline-formula> is reduced by this factor. Such convergence behavior we term superlinear. More concretely, for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x153.png" xlink:type="simple"/></inline-formula>, we obtain by the above method, using<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x154.png" xlink:type="simple"/></inline-formula>, starting with<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x148.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x149.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x150.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x151.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x152.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x153.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x154.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x155.png" xlink:type="simple"/></inline-formula>.</p><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x156.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula84"><label>(43a)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x157.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x158.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula85"><label>(43b)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x159.png"  xlink:type="simple"/></disp-formula><p>For <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/1-7403215x160.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.68151-formula86"><label>(43c)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/1-7403215x161.png"  xlink:type="simple"/></disp-formula></sec><sec id="s12"><title>12. Conclusions</title><p>The paper is predicated on the realistic assumption that the multiplicity index m of the iteratively targeted root is unknown. We conclude that if one prefers to shun second order derivatives, then the quadratic two-step method of Equation (29), that provides also ever better approximations for the multiplicity index m of the approached root, is a practically appealing alternative.</p><p>Otherwise, one may use the rational two-step method of Equation (34) with a constant k that is only slightly less than 2. Thus stating the method becomes superlinear, albeit, of a reduced speed of convergence for highly elevated root multiplicities. For the sake of brevity, the present paper does not explore the possibility of estimating the multiplicity index m of the sought root by the method of Equation (29), then applying this estimate to the choice of an optimal k in the method of Equations (34) and (35).</p></sec><sec id="s13"><title>Cite this paper</title><p>I. 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