<?xml version="1.0" encoding="UTF-8"?><!DOCTYPE article  PUBLIC "-//NLM//DTD Journal Publishing DTD v3.0 20080202//EN" "http://dtd.nlm.nih.gov/publishing/3.0/journalpublishing3.dtd"><article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink" dtd-version="3.0" xml:lang="en" article-type="research article"><front><journal-meta><journal-id journal-id-type="publisher-id">JAMP</journal-id><journal-title-group><journal-title>Journal of Applied Mathematics and Physics</journal-title></journal-title-group><issn pub-type="epub">2327-4352</issn><publisher><publisher-name>Scientific Research Publishing</publisher-name></publisher></journal-meta><article-meta><article-id pub-id-type="doi">10.4236/jamp.2017.52022</article-id><article-id pub-id-type="publisher-id">JAMP-74144</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>
 
 
  Euler-Maclaurin Expansions of Errors for Multidimensional Weakly Singular Integrals and Their Splitting Extrapolation Algorithm*
 
</article-title></title-group><contrib-group><contrib contrib-type="author" xlink:type="simple"><name name-style="western"><surname>Yubin</surname><given-names>Pan</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>Jin</surname><given-names>Huang</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>Hongyan</surname><given-names>Liu</given-names></name><xref ref-type="aff" rid="aff1"><sup>1</sup></xref></contrib></contrib-group><aff id="aff1"><addr-line>School of Mathematical Sciences, University of Electronic Science and Technology of China, Chengdu, China</addr-line></aff><pub-date pub-type="epub"><day>15</day><month>02</month><year>2017</year></pub-date><volume>05</volume><issue>02</issue><fpage>252</fpage><lpage>258</lpage><history><date date-type="received"><day>December</day>	<month>3,</month>	<year>2016</year></date><date date-type="rev-recd"><day>Accepted:</day>	<month>February</month>	<year>12,</year>	</date><date date-type="accepted"><day>February</day>	<month>15,</month>	<year>2017</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, multidimensional weakly singular integrals are solved by using rectangular quadrature rules which base on quadrature rules of one dimensional weakly singular and multidimensional regular integrals with their Euler-Maclaurin asymptotic expansions of the errors. The presented method is suit for solving multidimensional and singular integrals by comparing with Gauss quadrature rule. The error asymptotic expansions show that the convergence order of the initial quadrature rules is , where . The order of accuracy can reach to by using extrapolation and splitting extrapolation, where h0 is the maximum mesh width. Some numerical examples are constructed to show the efficiency of the method. 
  
 
</p></abstract><kwd-group><kwd>Multidimensional Weakly Singular Integrals</kwd><kwd> Euler-Maclaurin Errors  Asymptotic Expansions</kwd><kwd> Splitting Extrapolation</kwd></kwd-group></article-meta></front><body><sec id="s1"><title>1. Introduction</title><p>It is well known that multidimensional singular integrals are models arising in diverse engineering problems and mathematical applications. For example, in the boundary element fracture analysis problem, elasticity problem [<xref ref-type="bibr" rid="scirp.74144-ref1">1</xref>], bimaterial interfacial cracks [<xref ref-type="bibr" rid="scirp.74144-ref2">2</xref>] and wedge-sharped bimaterial interface [<xref ref-type="bibr" rid="scirp.74144-ref3">3</xref>], etc. Few of these integrals and equations can be solved explicitly, it is necessary to find a good numerical method. At present, there are many numerical techniques to calculate one-dimensional singular integrals or integral equations, such as collocation method [<xref ref-type="bibr" rid="scirp.74144-ref4">4</xref>], Gaussian quadrature method [<xref ref-type="bibr" rid="scirp.74144-ref5">5</xref>] [<xref ref-type="bibr" rid="scirp.74144-ref6">6</xref>], mechanical quadrature method [<xref ref-type="bibr" rid="scirp.74144-ref7">7</xref>] [<xref ref-type="bibr" rid="scirp.74144-ref8">8</xref>]. The Gauss-quadrature rules are considered to be a good choice for solving high dimensional integrals because they were accurate for polynomial approximation and the cost is low. However, Gaussian formula is not suitable for dealing with more than five-dimensional problems. So, we give a new algorithm for solving the following integral</p><disp-formula id="scirp.74144-formula109"><label>(1)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x6.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x7.png" xlink:type="simple"/></inline-formula>.</p><p>The structure of this paper is as follows: In Section 2, we give quadrature rules for weakly singular integral with multivariate errors asymptotic expansions. In Section 3, we construct the splitting extrapolation algorithm. In Section 4, some examples are given to illustrate the validity of the proposed method. Section 5 concludes the paper with a brief summary.</p></sec><sec id="s2"><title>2. Multi-Parameters Asymptotic Expansions of the Errors for Weakly Singular Integrals</title><p>In this part, we mainly consider multidimensional weakly singular integrals. We give the corresponding results of multidimensional weakly singular integrals according to the quadrature formula and asymptotic expansions of the errors of one-dimensional integrals.</p><p>Theorem 1. If <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x8.png" xlink:type="simple"/></inline-formula> on the interval<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x9.png" xlink:type="simple"/></inline-formula>, and</p><p>we assume that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x10.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x11.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x12.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x13.png" xlink:type="simple"/></inline-formula>,<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x14.png" xlink:type="simple"/></inline-formula>. Then we have the following asymptotic expansions of the errors</p><disp-formula id="scirp.74144-formula110"><label>(2)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x15.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x16.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x17.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x18.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x19.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x20.png" xlink:type="simple"/></inline-formula>.</p><p>Proof: We prove the theorem by the mathematic induction method. First, the conclusion is obvious right for<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x21.png" xlink:type="simple"/></inline-formula>. Now, we assume that the result also holds when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x22.png" xlink:type="simple"/></inline-formula>. Next, we just need to prove the case of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x21.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x22.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x23.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.74144-formula111"><label>(3)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x24.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x25.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x26.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x27.png" xlink:type="simple"/></inline-formula>are functions which are independent of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x25.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x26.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x27.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x28.png" xlink:type="simple"/></inline-formula>. The integral can be written as</p><disp-formula id="scirp.74144-formula112"><label>(4)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x29.png"  xlink:type="simple"/></disp-formula><p>we consider <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x30.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.74144-formula113"><label>(5)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x31.png"  xlink:type="simple"/></disp-formula><p>then <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x32.png" xlink:type="simple"/></inline-formula> can be represented as</p><disp-formula id="scirp.74144-formula114"><label>(6)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x33.png"  xlink:type="simple"/></disp-formula><p>We need to consider the following formula</p><disp-formula id="scirp.74144-formula115"><label>(7)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x34.png"  xlink:type="simple"/></disp-formula><p>we know the above equation is obviously right by induction. Next, we calculate <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x35.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.74144-formula116"><label>(8)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x36.png"  xlink:type="simple"/></disp-formula><p>The same as <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x37.png" xlink:type="simple"/></inline-formula> we can easy obtain</p><disp-formula id="scirp.74144-formula117"><label>(9)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x38.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74144-formula118"><label>(10)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x39.png"  xlink:type="simple"/></disp-formula><p>Now, we consider <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x40.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.74144-formula119"><label>(11)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x41.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74144-formula120"><label>(12)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x42.png"  xlink:type="simple"/></disp-formula><disp-formula id="scirp.74144-formula121"><label>(13)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x43.png"  xlink:type="simple"/></disp-formula><p>Now, we obtain the following equation by taking the <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x44.png" xlink:type="simple"/></inline-formula> and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x45.png" xlink:type="simple"/></inline-formula> <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x44.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x45.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x46.png" xlink:type="simple"/></inline-formula> into Equation (4)</p><disp-formula id="scirp.74144-formula122"><label>(14)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x47.png"  xlink:type="simple"/></disp-formula><p>where <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x48.png" xlink:type="simple"/></inline-formula> are constant which are independent of<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x49.png" xlink:type="simple"/></inline-formula>. The proof has been completed. <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x48.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x49.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x50.png" xlink:type="simple"/></inline-formula></p></sec><sec id="s3"><title>3. Splitting Extrapolation Algorithm</title><p>Now, we introduce the splitting extrapolation algorithm</p><disp-formula id="scirp.74144-formula123"><label>(15)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x51.png"  xlink:type="simple"/></disp-formula><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x52.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x52.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x53.png" xlink:type="simple"/></inline-formula>.</p><p>First, we have to eliminate the minimum term of the errors expansions. According to (2), we can easily find that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x54.png" xlink:type="simple"/></inline-formula>, <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x55.png" xlink:type="simple"/></inline-formula>are low order terms when<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x56.png" xlink:type="simple"/></inline-formula>. Assuming that<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x57.png" xlink:type="simple"/></inline-formula>, and we use splitting extra- polation in the direction of <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x54.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x55.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x56.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x57.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x58.png" xlink:type="simple"/></inline-formula></p><disp-formula id="scirp.74144-formula124"><label>(16)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x59.png"  xlink:type="simple"/></disp-formula><p>Then, we use <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x60.png" xlink:type="simple"/></inline-formula> and obtain the following equation</p><p><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x61.png" xlink:type="simple"/></inline-formula> 17)</p><p>where<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x62.png" xlink:type="simple"/></inline-formula>, and <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x62.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x63.png" xlink:type="simple"/></inline-formula> are</p><p>constants which are unrelated to<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x64.png" xlink:type="simple"/></inline-formula>. We can obtain higher accuracy and convergence order by repeating the above process.</p></sec><sec id="s4"><title>4. Examples</title><p>In this section, we give some examples to illustrate the efficiency of the proposed method.</p><p>Example 1. We consider the following <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x65.png" xlink:type="simple"/></inline-formula>-dimensional integral [<xref ref-type="bibr" rid="scirp.74144-ref9">9</xref>]</p><disp-formula id="scirp.74144-formula125"><label>(18)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x66.png"  xlink:type="simple"/></disp-formula><p>We give the numerical results of the splitting extrapolation of types 1 and 2 and Gauss quadrature methods. <xref ref-type="table" rid="table1">Table 1</xref> gives the relative error (RE) and CPU time for different dimension (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x67.png" xlink:type="simple"/></inline-formula>) and splitting times (<inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x67.png" xlink:type="simple"/></inline-formula><inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x68.png" xlink:type="simple"/></inline-formula>). From the <xref ref-type="table" rid="table1">Table 1</xref>, we can find that the splitting extrapolation method is suit for solving high dimensional integrals, and Gauss quadrature rule is difficult for solving more than five dimensional problems.</p><p>Example 2. we consider the following integral</p><disp-formula id="scirp.74144-formula126"><label>(19)</label><graphic position="anchor" xlink:href="http://html.scirp.org/file/74144x69.png"  xlink:type="simple"/></disp-formula><p>This is a high dimensional weakly singular integral which can be solved by splitting extrapolation algorithm. In <xref ref-type="table" rid="table2">Table 2</xref>, we give the absolute errors and convergence orders for splitting extrapolation of each step. From the table, we can find that the convergence order can reach to <inline-formula><inline-graphic xlink:href="http://html.scirp.org/file/74144x70.png" xlink:type="simple"/></inline-formula> by using splitting extrapolation twice, and the orders are coincide with the theoretical analysis. In <xref ref-type="fig" rid="fig1">Figure 1</xref>, we give the curves of absolute errors for each splitting extrapolation. From the Vertical direction, the images sink and the slopes of the curves increase with the increasing of the splitting times, which indicates that the errors decrease and the convergence orders increase. From the horizontal coordinate, the errors are reduced with the increasing of the node numbers. This shows that the splitting extrapolation not only enhance the numerical precision but also the order of accuracy.</p><table-wrap id="table1" ><label><xref ref-type="table" rid="table1">Table 1</xref></label><caption><title> Numerical results with errors and orders of accuracy for Example 2</title></caption><table><tbody><thead><tr><th align="center" valign="middle" >N<sub>1</sub> = ∙∙∙ = N<sub>7</sub></th><th align="center" valign="middle" >2<sup>2</sup></th><th align="center" valign="middle" >2<sup>3</sup></th><th align="center" valign="middle" >2<sup>4</sup></th><th align="center" valign="middle" >2<sup>5</sup></th></tr></thead><tr><td align="center" valign="middle" >ε<sub>0</sub></td><td align="center" valign="middle" >1.26e+01</td><td align="center" valign="middle" >8.86e+00</td><td align="center" valign="middle" >6.14e+00</td><td align="center" valign="middle" >4.23e+00</td></tr><tr><td align="center" valign="middle" >r<sub>0</sub></td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >2<sup>0.50</sup></td><td align="center" valign="middle" >2<sup>0.53</sup></td><td align="center" valign="middle" >2<sup>0.54</sup></td></tr><tr><td align="center" valign="middle" >ε<sub>1</sub></td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >1.66e−02</td><td align="center" valign="middle" >4.15e−03</td><td align="center" valign="middle" >1.04e−03</td></tr><tr><td align="center" valign="middle" >r<sub>1</sub></td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >2<sup>2.00</sup></td><td align="center" valign="middle" >2<sup>2.00</sup></td></tr><tr><td align="center" valign="middle" >ε<sub>2</sub></td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >1.26e−05</td><td align="center" valign="middle" >7.99e−07</td></tr><tr><td align="center" valign="middle" >r<sub>2</sub></td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >*</td><td align="center" valign="middle" >2<sup>4.00</sup></td></tr></tbody></table></table-wrap><table-wrap id="table2" ><label><xref ref-type="table" rid="table2">Table 2</xref></label><caption><title> The compare between SE and Gauss quadrature method</title></caption><table><tbody><thead><tr><th align="center" valign="middle"  rowspan="2"  >s</th><th align="center" valign="middle"  rowspan="2"  >m</th><th align="center" valign="middle"  colspan="2"  >Type 1</th><th align="center" valign="middle"  colspan="2"  >Type 2</th><th align="center" valign="middle"  colspan="2"  >Gauss</th></tr></thead><tr><td align="center" valign="middle" >RE</td><td align="center" valign="middle" >CPU(s)</td><td align="center" valign="middle" >RE</td><td align="center" valign="middle" >CPU(s)</td><td align="center" valign="middle" >RE</td><td align="center" valign="middle" >CPU(s)</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >5</td><td align="center" valign="middle" >7</td><td align="center" valign="middle" >8.6e−13</td><td align="center" valign="middle" >335</td><td align="center" valign="middle" >5.0e−9</td><td align="center" valign="middle" >336</td><td align="center" valign="middle" >1.0e−8</td><td align="center" valign="middle" >42</td></tr><tr><td align="center" valign="middle" >8</td><td align="center" valign="middle" >1.9e−13</td><td align="center" valign="middle" >947</td><td align="center" valign="middle" >1.2e−8</td><td align="center" valign="middle" >656</td><td align="center" valign="middle" >1.0e−9</td><td align="center" valign="middle" >&gt;9 h</td></tr><tr><td align="center" valign="middle"  rowspan="2"  >8</td><td align="center" valign="middle" >5</td><td align="center" valign="middle" >3.7e−7</td><td align="center" valign="middle" >618</td><td align="center" valign="middle" >3.7e−7</td><td align="center" valign="middle" >502</td><td align="center" valign="middle" >4.1e−8</td><td align="center" valign="middle" >11,283</td></tr><tr><td align="center" valign="middle" >6</td><td align="center" valign="middle" >9.7e−9</td><td align="center" valign="middle" >4056</td><td align="center" valign="middle" >9.4e−9</td><td align="center" valign="middle" >3092</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr><tr><td align="center" valign="middle"  rowspan="2"  >9</td><td align="center" valign="middle" >4</td><td align="center" valign="middle" >2.1e−5</td><td align="center" valign="middle" >176</td><td align="center" valign="middle" >2.1e−5</td><td align="center" valign="middle" >144</td><td align="center" valign="middle" >1.0e−3</td><td align="center" valign="middle" >&gt;8 h</td></tr><tr><td align="center" valign="middle" >5</td><td align="center" valign="middle" >8.5e−7</td><td align="center" valign="middle" >1544</td><td align="center" valign="middle" >8.6e−7</td><td align="center" valign="middle" >1197</td><td align="center" valign="middle" ></td><td align="center" valign="middle" ></td></tr></tbody></table></table-wrap><fig id="fig1"  position="float"><label><xref ref-type="fig" rid="fig1">Figure 1</xref></label><caption><title> The absolute errors of splitting extrapolation</title></caption><graphic mimetype="image"   position="float"  xlink:type="simple"  xlink:href="http://html.scirp.org/file/74144x71.png"/></fig></sec><sec id="s5"><title>5. Conclusion</title><p>In this paper, we give the quadrature formula with the asymptotic expansions of errors for solving multidimensional integrals with arbitrary points weakly singular. According to the asymptotic expansions of errors, we construct splitting extrapolation algorithm to improve the accuracy and the convergence order of the numerical results. By comparing the numerical results of our method with Gauss quadrature method, we can conclude that the splitting extrapolation method is efficient for solving high dimensional integral and weakly singular integrals. Next, we consider how to use the method to deal with boundary integral and differential equations.</p></sec><sec id="s6"><title>Acknowledgements</title><p>The authors are very grateful to the referees and editors. This work was partially supported by the financial support from National Natural Science Foundation of China (Grant no. 11371079).</p></sec><sec id="s7"><title>Cite this paper</title><p>Pan, Y.B., Huang, J. and Liu, H.Y. (2017) Euler-Maclaurin Expansions of Errors for Multidimensional Weakly Singular Integrals and Their Splitting Extrapolation Algorithm. Journal of Applied Mathematics and Physics, 5, 252- 258. https://doi.org/10.4236/jamp.2017.52022</p></sec><sec id="s8"><title>NOTES</title></sec></body><back><ref-list><title>References</title><ref id="scirp.74144-ref1"><label>1</label><mixed-citation publication-type="other" xlink:type="simple">Korsunsky, A.M. (2002) On the Use of Interpolative Quadratures for Hypersingular Integrals in Fracture Mechanics. 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