<?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">OJAppS</journal-id><journal-title-group><journal-title>Open Journal of Applied Sciences</journal-title></journal-title-group><issn pub-type="epub">2165-3917</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/ojapps.2013.32027</article-id><article-id pub-id-type="publisher-id">OJAppS-33373</article-id><article-categories><subj-group subj-group-type="heading"><subject>Articles</subject></subj-group><subj-group subj-group-type="Discipline-v2"><subject>Biomedical&amp;Life Sciences</subject><subject> Chemistry&amp;Materials Science</subject><subject> Computer Science&amp;Communications</subject><subject> Engineering</subject><subject> Physics&amp;Mathematics</subject></subj-group></article-categories><title-group><article-title>
 
 
  Modified Adomian Techniques Applied to Non-Linear Volterra Integral Equations
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>aifa</surname><given-names>H. Ali</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Fawzi</surname><given-names>Abdelwahid</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>Department of Mathematics, Faculty of Science, University of Benghazi, Benghazi, Libya</addr-line></aff><author-notes><corresp id="cor1">* E-mail:<email>fawziabd@hotmail.com(FA)</email>;</corresp></author-notes><pub-date pub-type="epub"><day>19</day><month>06</month><year>2013</year></pub-date><volume>03</volume><issue>02</issue><fpage>202</fpage><lpage>207</lpage><history><date date-type="received"><day>January</day>	<month>28,</month>	<year>2013</year></date><date date-type="rev-recd"><day>March</day>	<month>1,</month>	<year>2013</year>	</date><date date-type="accepted"><day>March</day>	<month>9,</month>	<year>2013</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 work, we studied the performance of modified techniques of Adomian method applied to non-linear Volterra integral equations of the second kind. This study shows that the modified techniques are reliable, efficient and easy to use through recursive relations that involve simple integrals. Furthermore, we found that the right choice and the proper implementation of the modified techniques reduce the computational difficulties and increase the speed of convergent, comparing with the standard Adomian method.
     
 
</p></abstract><kwd-group><kwd>Adomian Decomposition Method; Volterra Integral Equations</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>In recent years, many works have been focusing on the developing and applying of advanced and efficient methods for integral equations such as implicitly linear collocation methods [<xref ref-type="bibr" rid="scirp.33373-ref1">1</xref>], product integration method [<xref ref-type="bibr" rid="scirp.33373-ref2">2</xref>], Hermite-type collocation method [<xref ref-type="bibr" rid="scirp.33373-ref3">3</xref>] and analytical (semianalytical) techniques such as Adomian decomposition method [4,5]. In this work, we investigate the performance of modified techniques of Adomian decomposition method applied to non-linear Volterra integral equations of the second kind. This type of integral equations has the following form</p><disp-formula id="scirp.33373-formula132301"><label>. (1.1)</label><graphic position="anchor" xlink:href="7-2310136\ef68c9a7-7b76-43ec-809f-35f6aeb1320e.jpg"  xlink:type="simple"/></disp-formula><p>Equation (1.1) represents a nonlinear Volterra integral equation of second kind with unknown function <img src="7-2310136\9827490d-a20e-4e12-a69d-946f0b0a65cb.jpg" /> and <img src="7-2310136\cc59f02c-cf78-43a4-afbe-4bd895a95e67.jpg" /> is a non-linear function of<img src="7-2310136\860b491d-c296-4fa0-bf37-18dedd5c6757.jpg" />, and we assumed that, the kernel <img src="7-2310136\f75cdd60-08a4-4f43-85b7-11fd00681879.jpg" /> and the function <img src="7-2310136\0d34e7a4-aee6-4a62-ab03-391f1227c119.jpg" /> are analytical functions on <img src="7-2310136\d1b12ac4-9748-44af-b2b3-7d27bacf064e.jpg" /> and<img src="7-2310136\3b207d8f-2905-4f29-bfae-88a6cd20697b.jpg" />, respectively. Hence, Equation (1.1) classifies as a linear Volterra integral equation of second kind if <img src="7-2310136\f577ee79-6926-4148-a298-b6575b1ee65a.jpg" /> is a linear function of the unknown function<img src="7-2310136\d789b4ad-6d38-411d-963e-93850836a7af.jpg" />.</p></sec><sec id="s2"><title>2. Standard Adomian Method</title><p>The standard technique for the non-linear integral Equation (1.1), starts by decomposing <img src="7-2310136\d3ae354b-9bd6-4435-91b8-bf6ff1dd152b.jpg" /> into<img src="7-2310136\2f6544da-79eb-4703-9408-7d7ade045924.jpg" />, and assuming that</p><disp-formula id="scirp.33373-formula132302"><label>. (2.1)</label><graphic position="anchor" xlink:href="7-2310136\f1efb33d-2a15-4229-936c-0f8f6ec1939e.jpg"  xlink:type="simple"/></disp-formula><p>For the non-linear function<img src="7-2310136\aba5ef85-1b5e-411f-aea1-2bce0bddcd21.jpg" />, we set</p><disp-formula id="scirp.33373-formula132303"><label>(2.2)</label><graphic position="anchor" xlink:href="7-2310136\ed4f2ada-0ee4-490a-a27e-22064032d15f.jpg"  xlink:type="simple"/></disp-formula><p>In (2.2), <img src="7-2310136\638b0100-620d-4a26-b43c-df22ec80a49e.jpg" />, <img src="7-2310136\b488e611-0c08-4375-8a54-b1a60179cfe3.jpg" />are special polynomials known as Adomian polynomials. In ref. [<xref ref-type="bibr" rid="scirp.33373-ref6">6</xref>], close formulas of these polynomials, for any non-linear function<img src="7-2310136\e92565b1-ccab-4f20-890f-02a22f5e4266.jpg" />, introduced in the terms of the Kronecker delta<img src="7-2310136\b23b8814-8705-4448-9374-4174a92ecdd2.jpg" />. With<img src="7-2310136\acda19df-618a-400d-a455-dc235c754d13.jpg" />, these formulas for <img src="7-2310136\da406dd8-36a9-459b-9f00-f8babd773e70.jpg" /> read</p><disp-formula id="scirp.33373-formula132304"><label>(2.3)</label><graphic position="anchor" xlink:href="7-2310136\e8ac13a6-baf4-4428-ae07-a8bcd2f51570.jpg"  xlink:type="simple"/></disp-formula><p>where</p><p><img src="7-2310136\f44d1fb8-9049-42bd-ad6f-e5b231072de0.jpg" /></p><p>Now Equation (1.1) becomes,</p><disp-formula id="scirp.33373-formula132305"><label>, (2.4)</label><graphic position="anchor" xlink:href="7-2310136\058f6249-ab44-4668-b64d-f4ef717b8fb3.jpg"  xlink:type="simple"/></disp-formula><p>Now <img src="7-2310136\edd096d3-93d0-49fc-b8c1-6d578ceb7e28.jpg" /> and the <img src="7-2310136\bd87c7da-648b-4db5-8fbf-84c006b956ea.jpg" /> can be completely determined by using the recurrent formula</p><disp-formula id="scirp.33373-formula132306"><label>(2.5)</label><graphic position="anchor" xlink:href="7-2310136\dac32051-a136-47e8-a6ad-d4914d6f137c.jpg"  xlink:type="simple"/></disp-formula><p>Consequently the solution of the integral Equation (1.1), in a series form, can be immediately determined by using (2.5).</p><p>Recently, ref. [<xref ref-type="bibr" rid="scirp.33373-ref7">7</xref>] claims that the choice of the initial data <img src="7-2310136\3b969825-aa6a-49c7-aab5-87437b8a7532.jpg" /> plays an essential rule on improving the performance and the speed of the convergence of the Adomian method. Furthermore, for a complicated function<img src="7-2310136\81ce0fd9-c688-47de-99fc-bd7fec428e6a.jpg" />, we can see immediately from the recurrent Formula (2.5) that the standard Adomian method will encounter computational difficulties. To see that, we applied the recurrent Formula (2.5) on the nonlinear Volterra integral equation</p><disp-formula id="scirp.33373-formula132307"><label>. (2.6)</label><graphic position="anchor" xlink:href="7-2310136\00b43548-69c0-4f10-94ab-ff87cd9b6158.jpg"  xlink:type="simple"/></disp-formula><p>If we choose<img src="7-2310136\c6a5f2d6-1912-4149-a0c0-3a55524e6835.jpg" />, then the other components can be found from (2.5) as follows:</p><p><img src="7-2310136\39bfc46c-eeb5-47ce-a743-99b99d730937.jpg" /></p><p><img src="7-2310136\07e74c73-58a5-4854-b10e-485c9c91a2bf.jpg" /></p><p><img src="7-2310136\5e6b5d73-8f6d-465e-b331-2d9ebb615575.jpg" /></p><p>Note that, with the help of the Mathematica Packages, we can deduce that these calculations will lead to the exact solution<img src="7-2310136\d0a44bcd-a166-4f7f-89d0-c5d449b3e78a.jpg" />, which is quit hard to see immediately from the above calculations.</p></sec><sec id="s3"><title>3. Modified Techniques</title><p>To reduce the computational difficulties of the standard method and accelerate the convergence of this method, we introduce modified techniques of the standard Adomian method [8,9].</p><p>First Modified Technique:</p><p>In the first modified technique, we assume that the function <img src="7-2310136\7eb6b844-e7a5-4f52-b9fa-180aa9392f71.jpg" /> can be split as follows</p><disp-formula id="scirp.33373-formula132308"><label>. (3.1)</label><graphic position="anchor" xlink:href="7-2310136\40370075-c98e-4b93-b217-1701d15c351d.jpg"  xlink:type="simple"/></disp-formula><p>Based on this assumption, we can introduce a slight change for the choice of the components <img src="7-2310136\6b1397f5-396a-4821-a891-88a4b5733446.jpg" /> and <img src="7-2310136\c51a81d0-b8b0-4b0a-95f0-d8fd020ef6cd.jpg" /> as following</p><disp-formula id="scirp.33373-formula132309"><label>(3.2)</label><graphic position="anchor" xlink:href="7-2310136\f9c34718-0440-40f4-8138-a66b29a8b6a6.jpg"  xlink:type="simple"/></disp-formula><p>As we will see in the next section, this change reduces, the computational difficulties of finding other components and accelerate the convergence of the standard Adomian method procedure. Furthermore, the improvement of the standard Adomian decomposition method, uses the first modified recursive Formula (3.2), depends mainly on the splitting (3.1). In addition, we recommend, to apply the first modified technique, when <img src="7-2310136\a917d572-7f37-42d2-b491-fdce28da7395.jpg" /> is given in term of a polynomial or a combination of polynomial and trigonometric, or transcendental, functions.</p><p>Second Modified Technique:</p><p>The main idea of the second modified technique is replacing the non-homogeneous function <img src="7-2310136\9ea8d89b-8ad1-4e50-acb6-7565ec27dabd.jpg" /> by a series of infinite components. Ref. [<xref ref-type="bibr" rid="scirp.33373-ref9">9</xref>] expresses <img src="7-2310136\dc03f51f-4da7-4d51-bbd7-9bd5077d49c2.jpg" /> in term of the Taylor series and introduces the recursive formula</p><disp-formula id="scirp.33373-formula132310"><label>(3.3)</label><graphic position="anchor" xlink:href="7-2310136\c9d7eab3-2cd8-4f10-9394-94bcdadf71db.jpg"  xlink:type="simple"/></disp-formula><p>In (3.3),<img src="7-2310136\7e5964fe-5b0f-47a1-adc9-19243e41865f.jpg" />; <img src="7-2310136\ab3b2c16-e8df-4226-adbf-9a6b0e97be3c.jpg" />represents the Taylor series components of<img src="7-2310136\aadb0017-2e13-45be-9e4b-9257e1d05d65.jpg" />. Note that, it is easily to observe that the second modified recursive Formula (3.3) minimizes the size of the calculations which produced in the standard Adomian decomposition method. In addition, it is clear that the reduction in each iteration of (3.3), will ease the construction of Adomian polynomials for the non-linear term.</p></sec><sec id="s4"><title>4. Comparison Study</title><p>In this section, we compare the modified techniques against the standard Adomian decomposition method. To do that, let us study the following examples of non-linear Volterra integral equations.</p><p>Example 1: Consider the nonlinear Volterra integral equation</p><disp-formula id="scirp.33373-formula132311"><label>(4.1)</label><graphic position="anchor" xlink:href="7-2310136\1f10d13d-93cb-42d4-8dd7-208ae625c07a.jpg"  xlink:type="simple"/></disp-formula><p>To investigate the first modified technique, we split <img src="7-2310136\09900b11-e55b-408b-857a-00e3f0daa6ae.jpg" /> into two parts, say</p><disp-formula id="scirp.33373-formula132312"><label>. (4.2)</label><graphic position="anchor" xlink:href="7-2310136\3440cc58-aa6c-492f-85ed-29568be132af.jpg"  xlink:type="simple"/></disp-formula><p>The modified recursive Formula (3.2) reads</p><p><img src="7-2310136\58072fa1-6ea0-4948-9948-1cfdf24f3e51.jpg" />,</p><p><img src="7-2310136\b52e32bc-e7ea-4b8e-bccd-7c9a6633e7df.jpg" /></p><p>This implies<img src="7-2310136\8fd29cf5-5cd4-4255-a90b-f054c9affd1d.jpg" />, for<img src="7-2310136\ab2fa2d6-25c0-43ce-b1bb-4670b217b043.jpg" />. This leads to the exact solution <img src="7-2310136\db6211e8-5bfe-43ec-a2a2-2bc6cd8d9089.jpg" /> and hence by deploying the right splitting of<img src="7-2310136\45da17db-cebb-4409-9226-a1d5600547b7.jpg" />, we can avoid the calculation difficulties of Adomian polynomials required for the non-linear term as we will see later.</p><p>To investigate the second modified technique, let us first expand the function <img src="7-2310136\2f3b46b9-c64f-4b1b-9104-e6a6d9293740.jpg" /> in term of Taylor series expansion. This reads</p><disp-formula id="scirp.33373-formula132313"><label>(4.3)</label><graphic position="anchor" xlink:href="7-2310136\9e6fc152-8e68-4f12-926d-76ff59e85c04.jpg"  xlink:type="simple"/></disp-formula><p>Next, the second modified recursive Formula (3.3) gives</p><disp-formula id="scirp.33373-formula132314"><label>(4.4)</label><graphic position="anchor" xlink:href="7-2310136\9ddafe5f-bdd9-4816-8618-7a051f44f925.jpg"  xlink:type="simple"/></disp-formula><p>This leads to</p><disp-formula id="scirp.33373-formula132315"><label>(4.5)</label><graphic position="anchor" xlink:href="7-2310136\8bb0e384-1cf0-4e34-a970-202e0546ffe4.jpg"  xlink:type="simple"/></disp-formula><p>This is the Taylor series expansion of secx, where <img src="7-2310136\75fbfdad-96b4-4d74-9162-04e0cce76a87.jpg" /> represents the <img src="7-2310136\4e965c82-df8f-407e-913b-2641d98d5723.jpg" /> Euler number. This study shows that the second modified technique eases the construction of Adomian polynomials for the non-linear term and hence reduces each term of the recursive Formula (3.3). This also shows that the second modified technique, for some cases, improves the performance of the standard method.</p><p>To investigate the performance of the standard Adomian method, we use the recurrent Formula (2.5). For the integral Equation (4.1), this reads</p><disp-formula id="scirp.33373-formula132316"><label>(4.6)</label><graphic position="anchor" xlink:href="7-2310136\de09dfd0-a81e-4c3a-bf85-e9da257ce653.jpg"  xlink:type="simple"/></disp-formula><p>This leads to computational difficulties.</p><p>Example 2: Consider the nonlinear Volterra integral equation</p><disp-formula id="scirp.33373-formula132317"><label>(4.7)</label><graphic position="anchor" xlink:href="7-2310136\aa1a312e-a1ca-4831-a842-3179859e2873.jpg"  xlink:type="simple"/></disp-formula><p>To investigate the performance of the standard Adomian method, we use the recurrent Formula (2.5). For the integral Equation (4.7), this reads</p><disp-formula id="scirp.33373-formula132318"><label>(4.8)</label><graphic position="anchor" xlink:href="7-2310136\a45eabab-3a40-48c3-a79b-9516c869b045.jpg"  xlink:type="simple"/></disp-formula><p>To apply the first modified technique, we split <img src="7-2310136\dae35e82-1a58-481f-9747-7de8b23cf79c.jpg" /> into two parts, say</p><disp-formula id="scirp.33373-formula132319"><label>. (4.9)</label><graphic position="anchor" xlink:href="7-2310136\7793d800-726c-4946-9042-b35fb85e3c5b.jpg"  xlink:type="simple"/></disp-formula><p>The modified recursive Formula (3.2) reads</p><disp-formula id="scirp.33373-formula132320"><label>(4.10)</label><graphic position="anchor" xlink:href="7-2310136\e4e3311c-4029-4c9c-8c24-9fd469eb14bd.jpg"  xlink:type="simple"/></disp-formula><p>This implies that</p><disp-formula id="scirp.33373-formula132321"><label>, (4.11)</label><graphic position="anchor" xlink:href="7-2310136\f7d0656b-fac7-483c-b1d2-74c5a012d602.jpg"  xlink:type="simple"/></disp-formula><p>which leads to the exact solution<img src="7-2310136\6d5c5777-4ca9-4b25-af33-4d45cc07f06f.jpg" />.</p><p>To apply the second modified technique, let us first expand the function <img src="7-2310136\505999e0-e457-4b23-accc-558410d80b11.jpg" /> in term of Taylor series expansion, which reads</p><disp-formula id="scirp.33373-formula132322"><label>(4.12)</label><graphic position="anchor" xlink:href="7-2310136\508cb3a7-3a72-4c3c-a65a-48b66c4a6e19.jpg"  xlink:type="simple"/></disp-formula><p>Next, the second modified recursive Formula (3.3) gives</p><disp-formula id="scirp.33373-formula132323"><label>(4.13)</label><graphic position="anchor" xlink:href="7-2310136\357e9aa2-2b50-4fd6-a69e-394f62f521c1.jpg"  xlink:type="simple"/></disp-formula><p>This leads to the Taylor series of the exact solution<img src="7-2310136\5ea94098-6a28-45e6-8a41-b744acb8dbee.jpg" />.</p><p>Example 3: Consider the non-linear Volterra integral equation</p><disp-formula id="scirp.33373-formula132324"><label>(4.15)</label><graphic position="anchor" xlink:href="7-2310136\213d3920-c129-43e0-877b-6cd0d561c956.jpg"  xlink:type="simple"/></disp-formula><p>To investigate the performance, we first apply the modified technique. To do that, we split <img src="7-2310136\935aa253-2a20-4596-9dd9-1ac803f71762.jpg" /> into two parts, as</p><disp-formula id="scirp.33373-formula132325"><label>(4.16)</label><graphic position="anchor" xlink:href="7-2310136\74588d37-a229-4c18-b79c-e956683515a3.jpg"  xlink:type="simple"/></disp-formula><p>The modified recursive Formula (3.2) gives</p><p><img src="7-2310136\c03006f9-73c9-46c4-ac57-e85e9fd632f1.jpg" /></p><p><img src="7-2310136\c782e4ae-68c1-445a-85df-50b47d1b5d4e.jpg" /></p><p>This implies that</p><disp-formula id="scirp.33373-formula132326"><label>, (4.17)</label><graphic position="anchor" xlink:href="7-2310136\d18cfd25-6853-4294-830a-6ad85bcf4ea7.jpg"  xlink:type="simple"/></disp-formula><p>which leads to the exact solution <img src="7-2310136\e440bb6e-2ad3-4a7b-ac0c-af0e350a2da6.jpg" /></p><p>To apply the second modified technique, let us first expand the function <img src="7-2310136\274563fa-4170-49ea-a9da-c8ee4300d9f1.jpg" /> in term of Taylor series expansion. This reads</p><disp-formula id="scirp.33373-formula132327"><label>(4.18)</label><graphic position="anchor" xlink:href="7-2310136\86b62126-4752-460d-9c05-bfe74d3aaa22.jpg"  xlink:type="simple"/></disp-formula><p>Next, the second modified recursive Formula (3.3) gives</p><disp-formula id="scirp.33373-formula132328"><label>(4.19)</label><graphic position="anchor" xlink:href="7-2310136\17fa459f-4741-4977-93ed-90830bb90eb1.jpg"  xlink:type="simple"/></disp-formula><p>This leads to exact solution <img src="7-2310136\c1c2be55-d693-46c0-ba77-f5513dd0b673.jpg" /></p><p>To show the computational difficulties of the standard Adomian method, we use the recurrent Formula (2.5). For the integral Equation (4.15), this reads</p><p><img src="7-2310136\56affd65-817a-482b-b4ec-71a43ed759d0.jpg" /></p><p><img src="7-2310136\00f1cdbc-7af7-4411-84a3-c4945b24181d.jpg" /></p><p><img src="7-2310136\034bbfb1-75b4-416a-803c-00c8765d09f0.jpg" /></p><p>This gives</p><p><img src="7-2310136\c7e762d9-c971-4f42-8ba0-cba092116584.jpg" /></p><p>This shows, the computational difficulties of the standard Adomian decomposition method comparing with the modified techniques.</p></sec><sec id="s5"><title>5. Conclusion</title><p>In this work we showed the accuracy, applicability and simplicity of modified techniques of Adomian method applied to non-linear Volterra integral equations. A compression study against the standard Adomian method showed the applicability and the accuracy of the modified techniques. For the modified techniques, this study showed that the first modified technique requires choosing the right splitting of the function<img src="7-2310136\776403cf-1b76-46bd-a55a-83925a8434d9.jpg" />. Hence, by using the right splitting, we can avoid the calculation difficulties of using the Adomian polynomials required for the non-linear term. In addition, this study also showed that the second modified technique overcomes the difficulty of the splitting of the function <img src="7-2310136\f2bb882a-7f94-42f5-97b2-1aa7e2037a8f.jpg" /> and eases the difficulties construction of the Adomian polynomials required for the non-linear term.</p></sec><sec id="s6"><title>REFERENCES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.33373-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">H. 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