<?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">ICA</journal-id><journal-title-group><journal-title>Intelligent Control and Automation</journal-title></journal-title-group><issn pub-type="epub">2153-0653</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ica.2012.32021</article-id><article-id pub-id-type="publisher-id">ICA-19245</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Computer Science&amp;Communications</subject></subj-group></article-categories><title-group><article-title>
 
 
  The Bezier Control Points Method for Solving Delay Differential Equation
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>ateme</surname><given-names>Ghomanjani</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Mohammad</surname><given-names>Hadi Farahi</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Applied Mathematics, Ferdowsi University of Mashhad, Mashhad, Iran</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>fatemeghomanjani@gmail.com(AG)</email>;<email>farahi@math.um.ac.ir(MHF)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>23</day><month>05</month><year>2012</year></pub-date><volume>03</volume><issue>02</issue><fpage>188</fpage><lpage>196</lpage><history><date date-type="received"><day>December</day>	<month>19,</month>	<year>2011</year></date><date date-type="rev-recd"><day>January</day>	<month>30,</month>	<year>2012</year>	</date><date date-type="accepted"><day>February</day>	<month>9,</month>	<year>2012</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, Bezier surface form is used to find the approximate solution of delay differential equations (DDE’s). By using a recurrence relation and the traditional least square minimization method, the best control points of residual function can be found where those control points determine the approximate solution of DDE. Some examples are given to show efficiency of the proposed method.
 
</p></abstract><kwd-group><kwd>Bezier Control Points; Delay Differential Equation; Residual Function; Boundary Value Problem; Proportional Delays</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>Delay differential equations are type of differential equations where the time derivatives at the current time depend on the solution, and possibly its derivatives, at previous times. A class of such equations, which involve derivatives with delays as well as the solution itself has been called neutral DDEs over the past century (see [1, 2]).</p><p>The basic theory concerning the stable factors and works on fundamental theory, e.g., existence and uniqueness of solutions, was presented in [1,2]. Since then, DDE have been extensively studied in recent decades and a great number of monographs have been published including significant works on dynamics of DDEs by Hale and Lunel [<xref ref-type="bibr" rid="scirp.19245-ref3">3</xref>], on stability by Niculescu [<xref ref-type="bibr" rid="scirp.19245-ref4">4</xref>], and so on. The interest in study of DDEs is caused by the fact that many processes have time-delays and have been models for better representations by systems of DDEs in science, engineering, economics, etc. Such systems, however, are still not feasible to actively analyze and control precisely, thus, the study of systems of DDEs has actively been conducted over the recent decades (see [1, 2]).</p><p>In this paper, we show a novel strategy by using the Bezier curves to find the approximate solution for delay differential equations by Bezier curves. Other numerical methods for DDEs are available in (see [5-8]). In section 2 delay differential equations will be introduced. Example of Time-Delay System will be stated in section 3. In section 4 delay differential equations with proportional delay will be introduced. Bezier curves and degree elevation will be stated in Sections 5 and 6 respectively. In Section 7 solution of delay differential equation using Bezier control points presented and aforementioned method will be implemented on it. In section 8, solved numerical examples, showed the efficiency and reliability of the method. Finally, section 9 will give a conclusion briefly.</p></sec><sec id="s2"><title>2. Delay Differential Equations</title><p>Most delay differential equations that arise in population dynamics and epidemiology model intrinsically nonnegative quantities. Therefore it is important to establish that nonnegative initial data give rise to nonnegative solutions. Consider the following</p><disp-formula id="scirp.19245-formula154099"><label>(2.1)</label><graphic position="anchor" xlink:href="9-7900138\193e9bbe-e706-4885-b698-637be50e22a0.jpg"  xlink:type="simple"/></disp-formula><p>with a single delay h &gt; 0. Assume that <img src="9-7900138\b6806367-67c3-4e7d-aa99-132f796a446f.jpg" /> and <img src="9-7900138\4f76f94f-3b79-4af0-afa1-571d4bba4c1d.jpg" /> are continuous on R<sup>3</sup>. Let <img src="9-7900138\f054c1ea-7b4b-4998-9eda-916200922d9c.jpg" /> be given and let <img src="9-7900138\10994989-539f-49e1-8a8b-317795b66f0e.jpg" /> be continuous. We seek a solution <img src="9-7900138\c76d82f3-5cd2-48e8-b6cb-dab85a771d98.jpg" /> of (2.1) satisfying</p><disp-formula id="scirp.19245-formula154100"><label>(2.2)</label><graphic position="anchor" xlink:href="9-7900138\b4cc481d-bd05-4343-b298-8591b5d715c7.jpg"  xlink:type="simple"/></disp-formula><p>and satisfying (2.1) on <img src="9-7900138\3698ea22-b04e-4335-af4d-0f66b34cfd05.jpg" /> for some<img src="9-7900138\27c36fd7-89fc-42f7-b93d-c0b090a21cce.jpg" />. Note that we must interpret <img src="9-7900138\5557ba20-268d-4259-965a-3d7759c1a1e4.jpg" /> as the right-hand derivative at s.</p><p>Now, we present a typical example of physical systems that exhibit time-delay phenomena. The example selected in this section fit nicely into the model (2.1).</p></sec><sec id="s3"><title>3. Example of Time-Delay System</title><p>The existence of delays (or gestation lags) in economic systems is quite natural since there must be finite period of time following a decision for its effects to appear. In one model [<xref ref-type="bibr" rid="scirp.19245-ref9">9</xref>] of aggregate economy, we let <img src="9-7900138\d70d18ae-d76b-42aa-96c9-ca8de1c09fbe.jpg" /> be the income which can split into consumption<img src="9-7900138\bf79a1b3-8161-4aac-9c4d-7cbc9a0ea66d.jpg" />, investment <img src="9-7900138\6c39993f-45db-4fd4-9c20-f6538d29248a.jpg" /> and autonomous expenditure.</p><p>Thus</p><disp-formula id="scirp.19245-formula154101"><label>(3.1)</label><graphic position="anchor" xlink:href="9-7900138\74a6c2a1-0bf9-4de3-9fb6-19984e472b39.jpg"  xlink:type="simple"/></disp-formula><p>Define</p><disp-formula id="scirp.19245-formula154102"><label>(3.2)</label><graphic position="anchor" xlink:href="9-7900138\c6b075c4-1283-4510-9b5a-28b48209b6b2.jpg"  xlink:type="simple"/></disp-formula><p>where c is a consumption coefficient. From (3.1) we get</p><disp-formula id="scirp.19245-formula154103"><label>(3.3)</label><graphic position="anchor" xlink:href="9-7900138\84cfd86d-65e7-4acf-89d6-a3fbb2b50b4c.jpg"  xlink:type="simple"/></disp-formula><p>It is assumed that there is finite interval of time between ordering and delivery of capital equipment following a decision to invest <img src="9-7900138\3779800c-6afc-4e85-b951-5490d83e76c5.jpg" /> In terms of the stock of capital assets <img src="9-7900138\9f600e4d-b057-4a98-b3bd-64669e2fbc7b.jpg" /> we have</p><disp-formula id="scirp.19245-formula154104"><label>(3.4)</label><graphic position="anchor" xlink:href="9-7900138\e5c281c2-ab44-4424-bb60-eb506142a610.jpg"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.19245-formula154105"><label>(3.5)</label><graphic position="anchor" xlink:href="9-7900138\d014e022-ab15-4028-b609-ced62be04209.jpg"  xlink:type="simple"/></disp-formula><p>Economic rationale implies that <img src="9-7900138\6c9e07fd-9017-481a-b967-3fc5ac8a2e74.jpg" /> is determined by the rate of saving (proportional to<img src="9-7900138\2d375ac2-b8a0-4a25-9a2c-35fa2fef2c94.jpg" />) and by the capital stock<img src="9-7900138\18f69ee7-623a-48a3-bf54-60a19e977a36.jpg" />. This means that</p><disp-formula id="scirp.19245-formula154106"><label>(3.6)</label><graphic position="anchor" xlink:href="9-7900138\3aedb541-16f3-436b-9b6b-698496448816.jpg"  xlink:type="simple"/></disp-formula><p>where<img src="9-7900138\f1414a06-6255-416a-8b3b-f04c23234313.jpg" />, <img src="9-7900138\6326edaa-9268-415e-ba6a-27c8b8dbfdb9.jpg" />and ε is a trend factor. Combining (3.4) and (3.5), we obtain:</p><disp-formula id="scirp.19245-formula154107"><label>(3.7)</label><graphic position="anchor" xlink:href="9-7900138\f5451e82-c2ae-4f8e-a9b8-1fb153dd0792.jpg"  xlink:type="simple"/></disp-formula><p>By (3.3) and (3.7), we arrive at</p><disp-formula id="scirp.19245-formula154108"><label>(3.8)</label><graphic position="anchor" xlink:href="9-7900138\72320268-b7a1-4f8b-b15b-9f8bc6fb3518.jpg"  xlink:type="simple"/></disp-formula><p>Finally, it follows from (3.5), (3.6) and (3.8) that</p><disp-formula id="scirp.19245-formula154109"><label>(3.9)</label><graphic position="anchor" xlink:href="9-7900138\1b8fa60d-71d5-43c4-a823-64fd4669826f.jpg"  xlink:type="simple"/></disp-formula><p>which expresses the formation of the rate of delivery of the new equipment. This is a typical functional differential equation (FDE) of retarded type.</p></sec><sec id="s4"><title>4. Delay Differential Equations with Proportional Delay</title><p>In this paper, approximate analytical solutions with high accuracy can be obtained by carrying out in the Bezier control points method.</p><p>Consider the following neutral functional-differential equation with proportional delays (see [10-12]),</p><disp-formula id="scirp.19245-formula154110"><label>(4.1)</label><graphic position="anchor" xlink:href="9-7900138\4547e4d5-1e1a-40a2-bc8c-c09f07cd0fe8.jpg"  xlink:type="simple"/></disp-formula><p>with the initial conditions</p><disp-formula id="scirp.19245-formula154111"><label>(4.2)</label><graphic position="anchor" xlink:href="9-7900138\64c868f4-a73e-4afc-b4b1-f037aef7c531.jpg"  xlink:type="simple"/></disp-formula><p>Here, <img src="9-7900138\245db586-c1c2-4e39-a025-ee0802acc5cb.jpg" />and <img src="9-7900138\80d2ca29-2992-4521-878f-327ff9eb5506.jpg" /> are given analytical functions, and<img src="9-7900138\8529bfa7-7772-4867-a8b3-f65da5860340.jpg" />, <img src="9-7900138\ba7331f2-3373-4dee-84c8-7a3703c7e293.jpg" />, <img src="9-7900138\dcff52fa-7291-419c-bc5e-3b0ac274a59e.jpg" />, <img src="9-7900138\209fafc8-dc00-46e9-b1fd-55aa185cf0a3.jpg" />denote given constants with <img src="9-7900138\1914741d-cb58-42b3-b838-525a2b1a35ec.jpg" /></p><p>The existence and the uniqueness of the analytic solution of the multi-pantograph equation are proved in [<xref ref-type="bibr" rid="scirp.19245-ref13">13</xref>], the Dirichlet series solution is constructed, and the sufficient condition of the asymptotic stability for the analytic solution is obtained. It is proved that the θ-methods with a variable stepsize are asymptotically stable if <img src="9-7900138\51bad019-54bb-4984-8000-07dbcb72d24d.jpg" /></p><p>Some numerical examples are given to show the properties of the θ-methods.</p><p>In order to apply the Bezier control points method, we rewrite Equation (4.1) as</p><p><img src="9-7900138\af4d37f1-5a92-43bd-8887-14af9771f372.jpg" /></p><p>Neutral functional-differential equations with proportional delays represent a particular class of delay differential equation. Such functional-differential equations play an important role in the mathematical modeling of real world phenomena [<xref ref-type="bibr" rid="scirp.19245-ref14">14</xref>]. Obviously, most of these equations cannot be solved exactly. It is therefore necessary to design efficient numerical methods to approximate their solutions. Ishiwata et al. used the rational approximation method [<xref ref-type="bibr" rid="scirp.19245-ref15">15</xref>] and the collocation method [<xref ref-type="bibr" rid="scirp.19245-ref16">16</xref>] to compute numerical solutions of delay differential equations with proportional delays. Hu et al. [<xref ref-type="bibr" rid="scirp.19245-ref17">17</xref>] applied linear multistep methods to compute numerical solutions for neutral delay differential equations. Wang et al. obtained approximate solutions for neutral delay differential equations by continuous Runge-Kutta methods [<xref ref-type="bibr" rid="scirp.19245-ref18">18</xref>] and oneleg θ-methods [13,19].</p></sec><sec id="s5"><title>5. Bezier Curves</title><p>A Bezier curve of degree n can be defined as follows (see [<xref ref-type="bibr" rid="scirp.19245-ref19">19</xref>]):</p><disp-formula id="scirp.19245-formula154112"><label>(5.1)</label><graphic position="anchor" xlink:href="9-7900138\7a6f4272-fc77-4604-90da-0c05d1f75906.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7900138\d1f8aa67-f89d-47af-9ce3-7b780574efb6.jpg" /> are the Bernstein polynomials over the interval<img src="9-7900138\aa34f445-c853-43eb-b3c4-9450adef136d.jpg" />. The Bezier coefficient <img src="9-7900138\9da4eb98-d210-4ffb-b1cd-1018b28cb863.jpg" /> is called the control point (see <xref ref-type="fig" rid="fig1">Figure 1</xref>). In particular</p><disp-formula id="scirp.19245-formula154113"><label>(5.2)</label><graphic position="anchor" xlink:href="9-7900138\4ddf0aeb-2960-4d31-a7f9-3cafa6c0373f.jpg"  xlink:type="simple"/></disp-formula><p>If <img src="9-7900138\53a43c4a-fbf0-4969-94c4-a0fae13cb3a5.jpg" /> be a vector-valued polynomial, then <img src="9-7900138\147b7f33-ae01-4068-95d2-59584e8e5e63.jpg" /> is called a parametric Bezier curve. The control polygon of a Bezier curve comprise of the line segments <img src="9-7900138\1443adc3-b92a-4ac8-9d34-161d50a28bf1.jpg" /> <img src="9-7900138\631d47c6-7725-4692-bcf8-ee6d053d3bb7.jpg" />. If <img src="9-7900138\3abfdd5a-f604-419f-9e4d-f864e2a51745.jpg" /> is a scalar-valued polynomial, we call the function <img src="9-7900138\b3c7e73b-0c57-4349-b9a4-8029a8fccc96.jpg" /> an explicit Bezier curve by <img src="9-7900138\b8701601-8961-40f3-8b87-ec97efd420d9.jpg" /> (see [20,21]).</p></sec><sec id="s6"><title>6. Degree Elevation</title><p>Suppose we were designing with Bezier curve as described, and use a Bezier polygon of degree n to approximate the desired given shape. Suppose the degree polygon dose not feat neatly the desired shape.</p><p>One way to proceed in such a situation is to increase the flexibility of the polygon by adding another vertex (control point) to it. As a first step, one might want to add another vertex, yet leave the desired curve of the shape unchanged, this corresponds to raising the degree of the Bezier curve by one (see <xref ref-type="fig" rid="fig2">Figure 2</xref>). Therefore, we are looking for a curve with control vertices <img src="9-7900138\7fede9aa-87dc-4cea-851e-4a617403fdbb.jpg" /> that describes the same curve of the shape as the original polygon <img src="9-7900138\56039f70-8618-459c-8492-bde08d408385.jpg" /> (see [21-25] for more details).</p><p>We rewrite our given Bezier curve as</p><p><img src="9-7900138\ec53e86d-7dcd-4d06-8385-a95155477d7d.jpg" /></p><p>The upper index of the first sum may be extended to n + 1, since the corresponding term is zero. The summation indices of the second sum may be shifted to index 1 and n + 1, but one may choose the lower index zero since only a zero term is added. Thus we have</p><disp-formula id="scirp.19245-formula154114"><label>(6.1)</label><graphic position="anchor" xlink:href="9-7900138\6f6699b9-0fce-4976-b875-e78902201f2a.jpg"  xlink:type="simple"/></disp-formula><p>Combining both sums and computing coefficients</p><p>yields:</p><disp-formula id="scirp.19245-formula154115"><label>(6.2)</label><graphic position="anchor" xlink:href="9-7900138\1afa361f-68a5-4db5-82ad-2e621e27d4b4.jpg"  xlink:type="simple"/></disp-formula><p>where <img src="9-7900138\2807d9f3-5c24-493b-bb86-6bddd7ce45da.jpg" /> is the control point of the Bezier curve <img src="9-7900138\9ef05093-cfa9-4aaf-9049-96cb900848fe.jpg" /> when it is elevated to degree n + 1. Now, the new control polygon consists of n + 2 control points.</p></sec><sec id="s7"><title>7. Solution of Delay Differential Equation Using Bezier Control Points</title><p>Consider the following boundary value problem</p><disp-formula id="scirp.19245-formula154116"><label>(7.1)</label><graphic position="anchor" xlink:href="9-7900138\e5a0c2d2-cdb1-4e9a-80af-90a44a1c7251.jpg"  xlink:type="simple"/></disp-formula><p>where L is differential operator with proportional delay, <img src="9-7900138\11139c0d-465d-44b7-ba33-29c89bd6aaa9.jpg" />is also a polynomial in t, and <img src="9-7900138\d1f04653-a7d3-467f-ae27-01c6c86d132c.jpg" /> (k = 0, 1, &#183;&#183;&#183; , m) [<xref ref-type="bibr" rid="scirp.19245-ref26">26</xref>].</p><p>We propose to represent the approximate solution of (7.1) <img src="9-7900138\44cfb46a-f0b6-4510-a83c-5a5b01177868.jpg" />in Bezier form. The choice of the Bezier form rather than the B-spline form is due to the fact that the Bezier form is easier to symbolically carry out the operations of multiplication, comparison and degree elevation than B-spline form. We choose the sum of squares of the Bezier control points of the residual to be the measure quantity. Minimizing this quantity gives the approximate solution. So, the obvious spotlight is in the following, if the minimizing of the quantity is zero, so the residual function is zero, which implies that the solution is the exact solution. We call this approach the control-point-based method. The detailed steps of the method are as follows (see [<xref ref-type="bibr" rid="scirp.19245-ref24">24</xref>]):</p><p>• Step 1. Choose a degree n and symbolically express the solution <img src="9-7900138\efea73b6-a515-471e-9257-31addcf83344.jpg" /> in the degree <img src="9-7900138\61c3bbf4-a47a-4bd1-8395-f6050c04bdcb.jpg" /> Bezier form</p><disp-formula id="scirp.19245-formula154117"><label>(7.2)</label><graphic position="anchor" xlink:href="9-7900138\142de580-700d-4f82-ac1a-6833768c8921.jpg"  xlink:type="simple"/></disp-formula><p>where the control points <img src="9-7900138\95ea56b2-0b4e-41a4-93f9-272ccb739da0.jpg" /> are to be determined.</p><p>• Step 2. Substituting the approximate solution <img src="9-7900138\711f6490-4655-4661-8314-26471864d6c1.jpg" /> into the differential Equation (7.1), we gain the residual function</p><p><img src="9-7900138\e587411c-7745-425a-9d9d-2b9c7d18a8a3.jpg" /></p><p>This is a polynomial in t with degree ≤ k, where</p><p><img src="9-7900138\3d60f1bb-f5ec-4bf0-993c-7d06c7abf187.jpg" /></p><p>So the residual function <img src="9-7900138\59d57378-4624-4a8d-b3bc-ca81174f0bd3.jpg" /> can be expressed in Bezier form as well,</p><disp-formula id="scirp.19245-formula154118"><label>(7.3)</label><graphic position="anchor" xlink:href="9-7900138\446e01e3-2c7a-49e4-a1ea-606efd33fb18.jpg"  xlink:type="simple"/></disp-formula><p>where the control points <img src="9-7900138\d487a2b0-d13a-43a1-9b4a-46ac776fe7eb.jpg" /> are linear functions in the unknowns<img src="9-7900138\0c848d1d-ad4b-453f-95fa-ca7ee7fb1d7b.jpg" />. These functions are derived using the operations of multiplication, degree elevation and differentiation for Bezier form.</p><p>• Step 3. Construct the objective function <img src="9-7900138\f7c3909c-ae6b-4669-98a8-5b910d70f893.jpg" /> Then F is also a function of<img src="9-7900138\875876ca-9c68-4394-9e95-c5acd81308a9.jpg" />.</p><p>• Step 4. Solve the constrained optimization problem:</p><disp-formula id="scirp.19245-formula154119"><label>(7.4)</label><graphic position="anchor" xlink:href="9-7900138\5939af2f-074c-4015-95f9-04053aa85b8a.jpg"  xlink:type="simple"/></disp-formula><p>by some optimization techniques, such as Lagrange multipliers method, we can be used to solve (7.4).</p><p>• Step 5. Substituting the minimum solution back into (7.2) arrives at the approximate solution to the differential equation.</p></sec><sec id="s8"><title>8. Numerical Examples</title><p>In this part, we used the mentioned control-point-based method on Bezier control points to solve DDE’s and system of DDE’s.</p><p>Example 8.1. As a practical example, we consider Evens and Raslan [<xref ref-type="bibr" rid="scirp.19245-ref6">6</xref>] the following pantograph delay equation:</p><p><img src="9-7900138\bebc1569-dd7d-40f5-8005-1ac09e79fc7f.jpg" />.</p><p>The exact solution is<img src="9-7900138\5e17bbb1-1b90-4993-8302-279319fff715.jpg" />. Now we try to find a degree two approximate solution. Let</p><p><img src="9-7900138\8ab35c22-6c16-48dc-a5ba-6d3f3dc231fc.jpg" />.</p><p>Substituting it into the above delay differential equation gives <img src="9-7900138\b9c1b78e-a2d6-4a74-adf5-1eeac8fb682c.jpg" /> as:</p><p><img src="9-7900138\06cc8b88-2db0-4166-b332-e5e829f8712e.jpg" /></p><p>where</p><p><img src="9-7900138\80806b6b-999b-45fa-8903-c63fe96f1146.jpg" /></p><p>Then construct the function</p><p><img src="9-7900138\f583accc-473b-436d-a1de-6d1edbd7e5c0.jpg" /></p><p>Minimizing <img src="9-7900138\9d6fb0ec-ad34-4370-b21b-0add201d8299.jpg" /> with <img src="9-7900138\6e5b9d55-e3ad-4728-9a9e-0eedb4443313.jpg" /> and u(1) = a<sub>2</sub> = exp(1). We obtain</p><p><img src="9-7900138\756462a9-6422-43b7-9391-5482c5c341e5.jpg" />.</p><p>Thus the approximate solution is</p><p><img src="9-7900138\f7ed33ea-426b-491c-a2a0-2c8280ecee4b.jpg" />.</p><p>In <xref ref-type="fig" rid="fig3">Figure 3</xref> compare approximated and exact value of<img src="9-7900138\dfbc4160-93c1-41a8-89ea-26d0bd5d3368.jpg" />. <xref ref-type="fig" rid="fig4">Figure 4</xref> shows the residual function.</p><p>Example 8.2. Consider the previous example with degree raising in Bezier control points.</p><p>Let</p><disp-formula id="scirp.19245-formula154120"><graphic  xlink:href="9-7900138\1214ef94-bae4-4b7b-a28c-fc7b5bffbfdb.jpg"  xlink:type="simple"/></disp-formula><p>Substituting it into the delay differential equation leads to <img src="9-7900138\3d88411b-3ec7-42c3-9c6a-e33325e4d222.jpg" /> as:</p><p><img src="9-7900138\e708f79e-1b68-41f9-aa0a-f11c7482576c.jpg" /></p><p>Then construct the function</p><p><img src="9-7900138\5633de7e-ded2-49d8-bb94-097bd483b76b.jpg" /></p><p>and minimizing F with <img src="9-7900138\059760e2-d37b-43e1-94de-300bf8559fb6.jpg" /> and u(1) = a<sub>8</sub> = exp(1). We obtain</p><p><img src="9-7900138\0db4b5b0-f8f9-4237-8268-0100b8ad3260.jpg" /><img src="9-7900138\95ca8111-81ca-491b-98d0-1a9da4f276a0.jpg" /></p><p><img src="9-7900138\962c7fa2-b273-45f0-ab46-f3e74e47aa1c.jpg" /><img src="9-7900138\2def8a2a-e9fa-46e8-8f25-96521fc009c2.jpg" /></p><p><img src="9-7900138\77a2dabc-994d-4a49-8dcb-f13c7c7fa6b7.jpg" /><img src="9-7900138\38fab8ec-890d-4abf-8019-2d438bc6e0a9.jpg" /></p><p>and</p><p><img src="9-7900138\0d9c7bc0-3b89-4df5-b13d-8deb8a3e852a.jpg" /></p><p>Thus the approximate solution is</p><p><img src="9-7900138\d58afb6d-d4c8-469c-a945-6b4832e73844.jpg" /></p><p>In <xref ref-type="fig" rid="fig5">Figure 5</xref> compare approximated and exact value of<img src="9-7900138\1b9710dd-90be-48a0-8ecd-3dc138315995.jpg" />. <xref ref-type="fig" rid="fig6">Figure 6</xref> shows the residual function.</p><p>Example 8.3. Consider the following second order linear DDE (see [<xref ref-type="bibr" rid="scirp.19245-ref5">5</xref>]):</p><p><img src="9-7900138\bd702217-5e7a-4dfe-89e4-f0ff840b9e18.jpg" /></p><p>where<img src="9-7900138\eaeeadb3-cdd9-47d8-87ef-81985e97bd26.jpg" />, with initial conditions <img src="9-7900138\2e013f07-d13b-4eed-b7e0-a34ffacb2a7a.jpg" /> <img src="9-7900138\bcb84f0c-77da-4ab3-8616-eedb8b27985e.jpg" />, and the exact solution is<img src="9-7900138\ed3c9f05-8856-4755-ab0d-871f7c3786ab.jpg" />.</p><p>Let</p><p><img src="9-7900138\925cf8d3-7488-43a3-9288-9105cf95df27.jpg" /></p><p>By applying this algorithm, we obtain <img src="9-7900138\adfe003d-ba77-4213-b5ca-e0f5e74741df.jpg" /> <img src="9-7900138\da32e000-30f3-4d66-93a7-76624bdfe92e.jpg" /></p><p><img src="9-7900138\9dbd0463-c719-46b4-86ca-b0270f76e07a.jpg" /><img src="9-7900138\4463ed7d-129c-46f6-b41e-ed91abd12b1f.jpg" /><img src="9-7900138\0ae7c3b9-4a4e-4d63-b054-812f2d226ba4.jpg" /><img src="9-7900138\6cd8735b-84de-454c-97b7-c1b59e81af00.jpg" /><img src="9-7900138\8b79fa8b-945b-415e-bd28-9462e6f80c5b.jpg" /><img src="9-7900138\6513db79-cce9-4ae7-bb09-2b51b2a245bb.jpg" /></p><p>and<img src="9-7900138\76448602-266a-4f0b-9f20-c786e2688581.jpg" />. Thus the approximate solution is</p><disp-formula id="scirp.19245-formula154121"><graphic  xlink:href="9-7900138\dbd571b3-4a18-4edc-8e06-1faa86ce725e.jpg"  xlink:type="simple"/></disp-formula><p><xref ref-type="fig" rid="fig7">Figure 7</xref>, compares the exact and approximate solution of<img src="9-7900138\dc795d59-49af-450a-8e4a-5d0754220ea5.jpg" />. <xref ref-type="fig" rid="fig8">Figure 8</xref> shows the residual function.</p><p>Example 8.4. Consider the following second order linear DDE (see [<xref ref-type="bibr" rid="scirp.19245-ref10">10</xref>]):</p><disp-formula id="scirp.19245-formula154122"><graphic  xlink:href="9-7900138\fa4df1f8-dd03-4762-bcba-2befab38f11c.jpg"  xlink:type="simple"/></disp-formula><p>where the exact solution is<img src="9-7900138\5ed5a3f1-59f6-4da5-87f1-1ad34675a49f.jpg" />. Let</p><p><img src="9-7900138\88c459f6-abe3-47c2-91dd-ac4629480eb8.jpg" /></p><p>By applying this algorithm, we obtain <img src="9-7900138\9eed79e2-d99f-48fc-93e3-02c1907bbe19.jpg" /> <img src="9-7900138\6810b8d3-9e13-40e3-9ad1-db729e1d7061.jpg" /></p><p><img src="9-7900138\f2fb883d-7b11-467a-b873-1019588bf031.jpg" /><img src="9-7900138\d69b89e3-d6fc-4c51-9162-bcde2a7c9715.jpg" /><img src="9-7900138\232ea489-9410-4fbf-9381-529d04610bde.jpg" /><img src="9-7900138\0856e5ea-9880-4987-b975-d5c2d188c987.jpg" /><img src="9-7900138\99c9b8ea-b64d-4f0e-858e-4fbd10776733.jpg" /><img src="9-7900138\e41be04d-bf4e-4935-9922-bf0f6b081766.jpg" /></p><p>and<img src="9-7900138\fe67c64f-496c-4378-bb00-5b92b47705ff.jpg" />. Thus the approximate solution is</p><disp-formula id="scirp.19245-formula154123"><graphic  xlink:href="9-7900138\9cdcada0-a790-4082-adaf-f34be3823f55.jpg"  xlink:type="simple"/></disp-formula><p><xref ref-type="fig" rid="fig9">Figure 9</xref>, compares the exact and approximate solution of<img src="9-7900138\ac0acab4-931e-4dd6-8289-fe2e43fe563d.jpg" />. <xref ref-type="fig" rid="fig1">Figure 1</xref>0 shows the residual function.</p><p>Example 8.5. In this example the following first order linear DDE’s is considered (see [<xref ref-type="bibr" rid="scirp.19245-ref13">13</xref>]):</p><p><img src="9-7900138\99ca657a-c0bf-4e55-8042-54632a5290ae.jpg" /></p><p>Since <img src="9-7900138\c9d222f5-540e-474e-b809-114e390b1bfd.jpg" /> and<img src="9-7900138\204e7840-1578-4b20-89bf-2d334b3ae565.jpg" />, <img src="9-7900138\890504e3-2cac-4d65-9ec7-cc307c624f29.jpg" />has a jump at t = 0. The second derivative <img src="9-7900138\f87f8e73-5dcf-43b5-ad8b-360d5ef8d392.jpg" /></p><p><img src="9-7900138\59294fcd-ad28-4bc2-9f51-b48265860ac5.jpg" /></p><p>and therefore it has a jump at t = 1.</p><p>Now we try to find an approximate solution. Let</p><p><img src="9-7900138\d45e0b0e-0601-4358-9d4e-2628667ee273.jpg" />.</p><p>By applying this algorithm, we acquire<img src="9-7900138\d38bc890-ae95-4c53-9ae7-3956d1614fa3.jpg" />, <img src="9-7900138\200e9a5c-1a13-47bf-9c3b-dcb45126531a.jpg" />, <img src="9-7900138\df77009e-c752-4faf-9972-b84a3bc0e71c.jpg" />,<img src="9-7900138\ce637f6e-2786-4c9a-83b2-f59d68377126.jpg" />. Thus</p><p>the approximate solution is</p><disp-formula id="scirp.19245-formula154124"><graphic  xlink:href="9-7900138\f36aa2db-18f1-4903-8b98-1642d6b212f7.jpg"  xlink:type="simple"/></disp-formula><p><xref ref-type="fig" rid="fig1">Figure 1</xref>1 shows the approximate value of<img src="9-7900138\11d5ba1d-8b3b-49dc-b87d-73df1565a9f6.jpg" />.</p></sec><sec id="s9"><title>9. Conclusion</title><p>In this paper, we use the control-point-based method to solve delay differential equations. In this method, firstly,</p><p>the rough solution is expressed in Bezier form, then the residual function is minimized to find the best approximate solution. Some examples are given to verify the reliability and efficiency of the proposed method.</p></sec><sec id="s10"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.19245-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">G. Adomian and R. 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