<?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.2020.118052</article-id><article-id pub-id-type="publisher-id">AM-102504</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>
 
 
  The Adomian Decomposition Method for Solving Volterra-Fredholm Integral Equation Using Maple
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Hunida</surname><given-names>M. Malaikah</given-names></name><xref ref-type="aff" rid="aff1"><sub>1</sub></xref><xref ref-type="corresp" rid="cor1"><sup>*</sup></xref></contrib></contrib-group><aff id="aff1"><label>1</label><addr-line>Department of Mathematics, Faculty of Science, King Abdulaziz University, Jeddah, KSA</addr-line></aff><pub-date pub-type="epub"><day>17</day><month>08</month><year>2020</year></pub-date><volume>11</volume><issue>08</issue><fpage>779</fpage><lpage>787</lpage><history><date date-type="received"><day>19,</day>	<month>July</month>	<year>2020</year></date><date date-type="rev-recd"><day>24,</day>	<month>August</month>	<year>2020</year>	</date><date date-type="accepted"><day>27,</day>	<month>August</month>	<year>2020</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, Adomian decomposition method (ADM) is used to solve the Volterra-Fredholm integral equation. A number of examples have been presented to explain the numerical results, which is the comparison between the exact solution and the numerical solution, and it is found through the tables and the amount of error between the exact solution and the numerical solution, it is very small and almost non-existent and is also illustrated through the graph how the exact solution of completely applies to the numerical solution This proves the accuracy of the method, which is the Adomian decomposition method (ADM) for solving the Volterra Fredholm integral equation using Maple 18. And that this method is characterized by ease, speed and great accuracy in obtaining numerical results.
 
</p></abstract><kwd-group><kwd>Volterra-Fredholm Integral Equation</kwd><kwd> Adomian Decomposition Method</kwd><kwd> Maple18</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>The current research intends to the Adomian decomposition method for solving Volterra-Fredholm integral equation using Maple18.</p><p>Integral equations are the basic sciences in our real life, and they explain physical, chemical, engineering, and medical phenomena, and more than that, they contribute greatly to reaching analytical and numerical solutions to these phenomena in various areas of our lives [<xref ref-type="bibr" rid="scirp.102504-ref1">1</xref>] [<xref ref-type="bibr" rid="scirp.102504-ref2">2</xref>]. There are several studies of Adomian decomposition metod, convergence and accuracy of Adomian’s decomposition method for the solution of Lorenz equationsis studied in [<xref ref-type="bibr" rid="scirp.102504-ref3">3</xref>]. Solving Riccati differential equation using Adomian’s decomposition method is given in [<xref ref-type="bibr" rid="scirp.102504-ref4">4</xref>]. An adaptation of Adomian decomposition for numeric-analytic integration of strongly nonlinear and chaotic oscillatorsis studied in [<xref ref-type="bibr" rid="scirp.102504-ref5">5</xref>]. The extended Adomian decomposition method for fourth order boundary value problems is given in [<xref ref-type="bibr" rid="scirp.102504-ref6">6</xref>]. The use of the Adomian decomposition method for solving multipoint boundary value problems is mentioned in [<xref ref-type="bibr" rid="scirp.102504-ref7">7</xref>]. [<xref ref-type="bibr" rid="scirp.102504-ref8">8</xref>] developed a new algorithm for evaluating Adomian polynomials. [<xref ref-type="bibr" rid="scirp.102504-ref9">9</xref>] studied an efficient algorithm for the multivariable Adomian polynomials. [<xref ref-type="bibr" rid="scirp.102504-ref10">10</xref>] found convenient analytic recurrence algorithms for the Adomian polynomials. A review of the Adomian decomposition method and its applications to fractional differential equations is given in [<xref ref-type="bibr" rid="scirp.102504-ref11">11</xref>]. [<xref ref-type="bibr" rid="scirp.102504-ref12">12</xref>] covers a bibliography of the theory and applications of the Adomian decomposition method. We find that solutions of nonlinear integral equations are more difficult to solve than linear integral equations and there are many analytical and numerical methods for solving linear and nonlinear integral equations mentioned in the references [<xref ref-type="bibr" rid="scirp.102504-ref13">13</xref>] [<xref ref-type="bibr" rid="scirp.102504-ref14">14</xref>] [<xref ref-type="bibr" rid="scirp.102504-ref15">15</xref>] [<xref ref-type="bibr" rid="scirp.102504-ref16">16</xref>]. We discuss the numerical solution of the integral Volterra equation of the second type using an implicit trapezoidal [<xref ref-type="bibr" rid="scirp.102504-ref17">17</xref>] [<xref ref-type="bibr" rid="scirp.102504-ref18">18</xref>]. The Adomian decomposition method of the Fredholm integral equation of the second kind using MATLAB and Maple is demonstrated in [<xref ref-type="bibr" rid="scirp.102504-ref19">19</xref>]. The Adomian decomposition method was applied to solve the Fredholm integral equation of the second kind [<xref ref-type="bibr" rid="scirp.102504-ref20">20</xref>]. Also, Modified analysis method for solving the Volterra integral equation of the second kind using Maple is discussed in [<xref ref-type="bibr" rid="scirp.102504-ref21">21</xref>].</p><p>In this article we have applied the Adomian decomposition method used by using the Maple algorithm by applying this algorithm to different examples, including finding the approximate solution and then comparing it to the exact solution and finding out the amount of error between the approximate solution and the exact solution.</p><p>The main objective of this work is to use the Adomian decomposition method in solving the Volterra-Fredholm integral equation of the second kind using Maple18.</p><p>The paper is arranged as follows: In Section 2, the Adomian decomposition method; in Section 3, numerical examples are also considered to show the ability of the proposed method, and the conclusion is drawn in Section 4.</p></sec><sec id="s2"><title>2. The Adomian Decomposition Method</title><p>To clarify the basic idea of this method, we consider the following general non-linear differential equation:</p><p>u ( x ) = f ( x ) + λ 1 ∫ a x K 1 ( x , t ) u ( t ) d t + λ 2 ∫ a b K 2 ( x , t ) u ( t ) d t . (1)</p><p>where L is assumed invertible and L − 1 is an inverse operator.</p><p>The standard Adomian method defines the solution u ( x ) by the series</p><p>u ( x ) = ∑ n = 0 ∞ u n ( x ) . (2)</p><p>The modified decomposition method</p><p>u 0 ( x ) = f ( x ) (3)</p><p>u 1 ( x ) = f ( x ) + L − 1 ( λ 1 ∫ a x K 1 ( x , t ) u 0 ( t ) d t ) + L − 1 ( λ 2 ∫ a b K 2 ( x , t ) u 0 ( t ) d t ) , (4)</p><p>u n + 1 ( x ) = L − 1 ( λ 1 ∫ a x K 1 ( x , t ) u n ( t ) d t ) + L − 1 ( λ 2 ∫ a b K 2 ( x , t ) u n ( t ) d t ) . (5)</p><p>The use of a modified decomposition method not only reduces the calculations but avoids the use of the human polynomial arrangement of boundaries in such cases.</p></sec><sec id="s3"><title>3. Numerical Examples</title><p>In this section, we solve some examples, and we can compare the numerical results with the exact solution.</p><p>Example 1. Consider the Volterra Fredholm integral equation</p><p>u ( x ) = x − 1 3 x 3 + ∫ 0 x t u ( t ) d t + ∫ − 1 1 t 2 u ( t ) d t , (6)</p><p>the exact Solution u ( x ) = x .</p><p>Applying the Adomian decomposition method using Maple18 we find (<xref ref-type="table" rid="table1">Table 1</xref> &amp; <xref ref-type="fig" rid="fig1">Figure 1</xref>).</p><p>Example 2. Consider the Volterra Fredholm integral equation</p><p>u ( x ) = sin ( x ) − cos ( x ) − ∫ 0 x u ( t ) d t + ∫ 0 π 2 u ( t ) d t (7)</p><p>the exact Solution u ( x ) = sin ( x ) .</p><p>Applying the Adomian Decomposition Method using Maple18 we find (<xref ref-type="table" rid="table2">Table 2</xref> &amp; <xref ref-type="fig" rid="fig2">Figure 2</xref>).</p><p>Example 3. Consider the Volterra Fredholm integral equation</p><p>u ( x ) = 3 x + 4 x 2 − x 3 − x 4 − 2 + ∫ 0 x t u ( t ) d t + ∫ − 1 1 t u ( t ) d t . (8)</p><p>the exact Solution u ( x ) = 3 x + 4 x 2 .</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Approximation solution and exact solution of Volterra Fredholm integral equations for example 1</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >x</th><th align="center" valign="middle" >u = x</th><th align="center" valign="middle" >Exact 1 = x</th><th align="center" valign="middle" >Error = | Exact 1 − u |</th></tr></thead><tr><td align="center" valign="middle" >0.10000</td><td align="center" valign="middle" >0.1000000</td><td align="center" valign="middle" >0.1000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.20000</td><td align="center" valign="middle" >0.2000000</td><td align="center" valign="middle" >0.2000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.30000</td><td align="center" valign="middle" >0.3000000</td><td align="center" valign="middle" >0.3000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.40000</td><td align="center" valign="middle" >0.4000000</td><td align="center" valign="middle" >0.4000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.50000</td><td align="center" valign="middle" >0.5000000</td><td align="center" valign="middle" >0.5000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.60000</td><td align="center" valign="middle" >0.6000000</td><td align="center" valign="middle" >0.6000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.70000</td><td align="center" valign="middle" >0.7000000</td><td align="center" valign="middle" >0.7000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.80000</td><td align="center" valign="middle" >0.8000000</td><td align="center" valign="middle" >0.8000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >0.90000</td><td align="center" valign="middle" >0.9000000</td><td align="center" valign="middle" >0.9000000</td><td align="center" valign="middle" >0.0000000</td></tr><tr><td align="center" valign="middle" >1.00000</td><td align="center" valign="middle" >1.0000000</td><td align="center" valign="middle" >1.0000000</td><td align="center" valign="middle" >0.0000000</td></tr></tbody></table></table-wrap><table-wrap-group id="2"><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> Approximation solution and exact solution of Volterra Fredholm integral equations for example 2</title></caption><table-wrap id="2_1"><table><tbody><thead><tr><th align="center" valign="middle" >Error = | Exact 2 − u |</th><th align="center" valign="middle" >Exact 2 = sin ( x )</th><th align="center" valign="middle" >u</th><th align="center" valign="middle" >x</th></tr></thead><tr><td align="center" valign="middle" >0.0000870</td><td align="center" valign="middle" >0.0998334</td><td align="center" valign="middle" >0.0997464</td><td align="center" valign="middle" >0.10000</td></tr><tr><td align="center" valign="middle" >0.0000463</td><td align="center" valign="middle" >0.1986693</td><td align="center" valign="middle" >0.1986230</td><td align="center" valign="middle" >0.20000</td></tr></tbody></table></table-wrap><table-wrap id="2_2"><table><tbody><thead><tr><th align="center" valign="middle" >0.0000235</th><th align="center" valign="middle" >0.2955202</th><th align="center" valign="middle" >0.2954967</th><th align="center" valign="middle" >0.30000</th></tr></thead><tr><td align="center" valign="middle" >0.0000113</td><td align="center" valign="middle" >0.3894183</td><td align="center" valign="middle" >0.3894071</td><td align="center" valign="middle" >0.40000</td></tr><tr><td align="center" valign="middle" >0.0000050</td><td align="center" valign="middle" >0.4794255</td><td align="center" valign="middle" >0.4794205</td><td align="center" valign="middle" >0.50000</td></tr><tr><td align="center" valign="middle" >0.0000021</td><td align="center" valign="middle" >0.5646425</td><td align="center" valign="middle" >0.5646404</td><td align="center" valign="middle" >0.60000</td></tr><tr><td align="center" valign="middle" >0.0000008</td><td align="center" valign="middle" >0.6442177</td><td align="center" valign="middle" >0.6442169</td><td align="center" valign="middle" >0.70000</td></tr><tr><td align="center" valign="middle" >0.0000003</td><td align="center" valign="middle" >0.7173561</td><td align="center" valign="middle" >0.7173558</td><td align="center" valign="middle" >0.80000</td></tr><tr><td align="center" valign="middle" >0.0000001</td><td align="center" valign="middle" >0.7833269</td><td align="center" valign="middle" >0.7833268</td><td align="center" valign="middle" >0.90000</td></tr><tr><td align="center" valign="middle" >0.0000000</td><td align="center" valign="middle" >0.8414710</td><td align="center" valign="middle" >0.8414710</td><td align="center" valign="middle" >1.00000</td></tr></tbody></table></table-wrap></table-wrap-group><table-wrap id="table3" ><label><xref ref-type="table" rid="table3">Table 3</xref></label><caption><title> Approximation solution and exact solution of Volterra Fredholm integral equations for example 3</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Error = | Exact 3 − u |</th><th align="center" valign="middle" >Exact 3 = 3 x + 4 x 2</th><th align="center" valign="middle" >u</th><th align="center" valign="middle" >x</th></tr></thead><tr><td align="center" valign="middle" >0.0000002</td><td align="center" valign="middle" >0.3399998</td><td align="center" valign="middle" >0.3400000</td><td align="center" valign="middle" >0.10000</td></tr><tr><td align="center" valign="middle" >0.0000002</td><td align="center" valign="middle" >0.7599998</td><td align="center" valign="middle" >0.7600000</td><td align="center" valign="middle" >0.20000</td></tr><tr><td align="center" valign="middle" >0.0000004</td><td align="center" valign="middle" >1.2599996</td><td align="center" valign="middle" >1.2600000</td><td align="center" valign="middle" >0.30000</td></tr><tr><td align="center" valign="middle" >0.0000006</td><td align="center" valign="middle" >1.8399994</td><td align="center" valign="middle" >1.8400000</td><td align="center" valign="middle" >0.40000</td></tr><tr><td align="center" valign="middle" >0.0000012</td><td align="center" valign="middle" >2.4999988</td><td align="center" valign="middle" >2.5000000</td><td align="center" valign="middle" >0.50000</td></tr><tr><td align="center" valign="middle" >0.0000024</td><td align="center" valign="middle" >3.2399976</td><td align="center" valign="middle" >3.2400000</td><td align="center" valign="middle" >0.60000</td></tr><tr><td align="center" valign="middle" >0.0000052</td><td align="center" valign="middle" >4.0599948</td><td align="center" valign="middle" >4.0600000</td><td align="center" valign="middle" >0.70000</td></tr><tr><td align="center" valign="middle" >0.0000117</td><td align="center" valign="middle" >4.9599883</td><td align="center" valign="middle" >4.9600000</td><td align="center" valign="middle" >0.80000</td></tr><tr><td align="center" valign="middle" >0.0000269</td><td align="center" valign="middle" >5.9399731</td><td align="center" valign="middle" >5.9400000</td><td align="center" valign="middle" >0.90000</td></tr><tr><td align="center" valign="middle" >0.0000625</td><td align="center" valign="middle" >6.9999375</td><td align="center" valign="middle" >7.0000000</td><td align="center" valign="middle" >1.00000</td></tr></tbody></table></table-wrap><p>Applying the Adomian Decomposition Method using Maple18 we find (<xref ref-type="table" rid="table3">Table 3</xref> &amp; <xref ref-type="fig" rid="fig3">Figure 3</xref>).</p><p>Example 4. Consider the Volterra Fredholm integral equation</p><p>u ( x ) = − 2 − 2 x + 2 e x + ∫ 0 x ( x − t ) u ( t ) d t + ∫ 0 1 x u ( t ) d t (9)</p><p>the exact Solution u ( x ) = x e x .</p><p>Applying the Adomian Decomposition Method using Maple we find (<xref ref-type="table" rid="table4">Table 4</xref> &amp; <xref ref-type="fig" rid="fig4">Figure 4</xref>).</p><p>Example 5. Consider the Volterra Fredholm integral equation</p><p>u ( x ) = x 3 − 9 20 x 5 − 1 4 x + 1 5 + ∫ 0 x ( x + t ) u ( t ) d t + ∫ 0 1 ( x − t ) u ( t ) d t (10)</p><p>the exact Solution u ( x ) = x 3 .</p><table-wrap id="table4" ><label><xref ref-type="table" rid="table4">Table 4</xref></label><caption><title> Approximation solution and exact solution of Volterra Fredholm integral equations for example 4</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Error = | Exact 4 − u |</th><th align="center" valign="middle" >Exact 4 = x e x</th><th align="center" valign="middle" >u</th><th align="center" valign="middle" >x</th></tr></thead><tr><td align="center" valign="middle" >0.0011984</td><td align="center" valign="middle" >0.1093187</td><td align="center" valign="middle" >0.1105171</td><td align="center" valign="middle" >0.10000</td></tr><tr><td align="center" valign="middle" >0.0024176</td><td align="center" valign="middle" >0.2418630</td><td align="center" valign="middle" >0.2442806</td><td align="center" valign="middle" >0.20000</td></tr><tr><td align="center" valign="middle" >0.0036788</td><td align="center" valign="middle" >0.4012789</td><td align="center" valign="middle" >0.4049576</td><td align="center" valign="middle" >0.30000</td></tr><tr><td align="center" valign="middle" >0.0050039</td><td align="center" valign="middle" >0.5917260</td><td align="center" valign="middle" >0.5967299</td><td align="center" valign="middle" >0.40000</td></tr><tr><td align="center" valign="middle" >0.0064158</td><td align="center" valign="middle" >0.8179448</td><td align="center" valign="middle" >0.8243606</td><td align="center" valign="middle" >0.50000</td></tr><tr><td align="center" valign="middle" >0.0079393</td><td align="center" valign="middle" >1.0853320</td><td align="center" valign="middle" >1.0932713</td><td align="center" valign="middle" >0.60000</td></tr><tr><td align="center" valign="middle" >0.0096006</td><td align="center" valign="middle" >1.4000262</td><td align="center" valign="middle" >1.4096269</td><td align="center" valign="middle" >0.70000</td></tr><tr><td align="center" valign="middle" >0.0114287</td><td align="center" valign="middle" >1.7690040</td><td align="center" valign="middle" >1.7804327</td><td align="center" valign="middle" >0.80000</td></tr><tr><td align="center" valign="middle" >0.0134553</td><td align="center" valign="middle" >2.2001875</td><td align="center" valign="middle" >2.2136428</td><td align="center" valign="middle" >0.90000</td></tr><tr><td align="center" valign="middle" >0.0157157</td><td align="center" valign="middle" >2.7025662</td><td align="center" valign="middle" >2.7182818</td><td align="center" valign="middle" >1.00000</td></tr></tbody></table></table-wrap><table-wrap id="table5" ><label><xref ref-type="table" rid="table5">Table 5</xref></label><caption><title> Approximation solution and exact solution of Volterra Fredholm integral equations for example 5</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >Error = | Exact 5 − u |</th><th align="center" valign="middle" >Exact 5 = x 3</th><th align="center" valign="middle" >u</th><th align="center" valign="middle" >x</th></tr></thead><tr><td align="center" valign="middle" >0.0002218</td><td align="center" valign="middle" >0.0007782</td><td align="center" valign="middle" >0.0010000</td><td align="center" valign="middle" >0.10000</td></tr><tr><td align="center" valign="middle" >0.0003499</td><td align="center" valign="middle" >0.0083499</td><td align="center" valign="middle" >0.0080000</td><td align="center" valign="middle" >0.20000</td></tr><tr><td align="center" valign="middle" >0.0010883</td><td align="center" valign="middle" >0.0280883</td><td align="center" valign="middle" >0.0270000</td><td align="center" valign="middle" >0.30000</td></tr><tr><td align="center" valign="middle" >0.0019947</td><td align="center" valign="middle" >0.0659947</td><td align="center" valign="middle" >0.0640000</td><td align="center" valign="middle" >0.40000</td></tr><tr><td align="center" valign="middle" >0.0030596</td><td align="center" valign="middle" >0.1280596</td><td align="center" valign="middle" >0.1250000</td><td align="center" valign="middle" >0.50000</td></tr><tr><td align="center" valign="middle" >0.0042426</td><td align="center" valign="middle" >0.2202426</td><td align="center" valign="middle" >0.2160000</td><td align="center" valign="middle" >0.60000</td></tr><tr><td align="center" valign="middle" >0.0054413</td><td align="center" valign="middle" >0.3484413</td><td align="center" valign="middle" >0.3430000</td><td align="center" valign="middle" >0.70000</td></tr><tr><td align="center" valign="middle" >0.0064507</td><td align="center" valign="middle" >0.5184507</td><td align="center" valign="middle" >0.5120000</td><td align="center" valign="middle" >0.80000</td></tr><tr><td align="center" valign="middle" >0.0069143</td><td align="center" valign="middle" >0.7359143</td><td align="center" valign="middle" >0.7290000</td><td align="center" valign="middle" >0.90000</td></tr><tr><td align="center" valign="middle" >0.0062804</td><td align="center" valign="middle" >1.0062804</td><td align="center" valign="middle" >1.0000000</td><td align="center" valign="middle" >1.00000</td></tr></tbody></table></table-wrap><p>Applying the Adomian Decomposition Method using Maple18 we find (<xref ref-type="table" rid="table5">Table 5</xref> &amp; <xref ref-type="fig" rid="fig5">Figure 5</xref>).</p></sec><sec id="s4"><title>4. Conclusion</title><p>In this paper, the Adomian decomposition method was applied to solve the integral Volterra Fredholm equation using program Maple18. The results are obtained in the tables and drawn in the figures. Tables 1-5 show the correct solution and the numerical solution. Tables 1-5 represent the exact and numerical results of the examples in this article. Figures 1-5 readily show the comparison of exact solution and ap-proximate solution. Comparing the numerical results, we find that the numerical solution is largely applied to the exact solution, which proves the efficiency of the method used and the ability to obtain the numerical solution corresponding to the exact solution easily and conveniently with a program Maple 18. Moreover, the high accuracy of the results is obtained.</p></sec><sec id="s5"><title>Acknowledgements</title><p>This project was funded by the Deanship of Scientific Research (DSR), King Abdulaziz University. The author, therefore, acknowledges with thanks for DSR technical and fnancial support.</p></sec><sec id="s6"><title>Conflicts of Interest</title><p>The author declares no conflicts of interest regarding the publication of this paper.</p></sec><sec id="s7"><title>Cite this paper</title><p>Malaikah, H.M. (2020) The Adomian Decomposition Method for Solving Volterra-Fredholm Integral Equation Using Maple. Applied Mathematics, 11, 779-787. https://doi.org/10.4236/am.2020.118052</p></sec></body><back><ref-list><title>References</title><ref id="scirp.102504-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Abdul-Majid, W. (1999) A Reliable Modification of Adomain Decomposition Method. Applied Mathematics and Computation, 102, 77-86. https://doi.org/10.1016/S0096-3003(98)10024-3</mixed-citation></ref><ref id="scirp.102504-ref2"><label>2</label><mixed-citation publication-type="other" xlink:type="simple">Wazwaz, A.-M. and El-Sayed, S.M. 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