On uniqueness of numerical solution of boundary integral equations with 3-times monotone radial kernels

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• 作者：Zeynab Sedaghatjoo^a ; ^{z.sedaqatjoo@aut.ac.ir" class="auth_mail" title="E-mail the corresponding author} ; ^{zeinab.sedaghatjoo@gmail.com" class="auth_mail" title="E-mail the corresponding author} ; Mehdi Dehghan^a ; ^{mdehghan@aut.ac.ir" class="auth_mail" title="E-mail the corresponding author} ; ^{mdehghan.aut@gmail.com" class="auth_mail" title="E-mail the corresponding author} ; Hossein Hosseinzadeh^b ; ^{h_hosseinzadeh@aut.ac.ir" class="auth_mail" title="E-mail the corresponding author} ; ^{hosseinzadeh@pgu.ac.ir" class="auth_mail" title="E-mail the corresponding author}
• 关键词：65N38 ; 45B05 ; 65Z99 ; 65M70 ; 65R20
• 刊名：Journal of Computational and Applied Mathematics
• 出版年：2017
• 出版时间：February 2017
• 年：2017
• 卷：311
• 期：Complete
• 页码：664-681
• 全文大小：858 K

文摘

The uniqueness of solution of boundary integral equations (BIEs) is studied here when geometry of boundary and unknown functions are assumed piecewise constant. In fact we will show BIEs with 3-times monotone radial kernels have unique piecewise constant solution. In this paper nonnegative radial function mmlsi76" class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303910&_mathId=si76.gif&_user=111111111&_pii=S0377042716303910&_rdoc=1&_issn=03770427&md5=f815f3e4f6250c972ae978c02ae9fc4a" title="Click to view the MathML source">F^δ₃class="mathContainer hidden">class="mathCode"><math altimg="si76.gif" overflow="scroll"><msup><mrow><mi mathvariant="script">Fmi>mrow><mrow><msub><mrow><mi>δmi>mrow><mrow><mn>3mn>mrow>msub>mrow>msup>math> is introduced which has important contribution in proving the uniqueness. It can be found from the paper if mmlsi77" class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303910&_mathId=si77.gif&_user=111111111&_pii=S0377042716303910&_rdoc=1&_issn=03770427&md5=0db60c1dda28e808aa115f522e3fb861" title="Click to view the MathML source">δ₃class="mathContainer hidden">class="mathCode"><math altimg="si77.gif" overflow="scroll"><msub><mrow><mi>δmi>mrow><mrow><mn>3mn>mrow>msub>math> is sufficiently small then eigenvalues of the boundary integral operator are bigger than mmlsi78" class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303910&_mathId=si78.gif&_user=111111111&_pii=S0377042716303910&_rdoc=1&_issn=03770427&md5=6e6d41c38be23b3f87b2bf05a18a2eb0" title="Click to view the MathML source">F^δ₃/2class="mathContainer hidden">class="mathCode"><math altimg="si78.gif" overflow="scroll"><msup><mrow><mi mathvariant="script">Fmi>mrow><mrow><msub><mrow><mi>δmi>mrow><mrow><mn>3mn>mrow>msub>mrow>msup><mo>/mo><mn>2mn>math>. Note that there is a smart relation between mmlsi77" class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303910&_mathId=si77.gif&_user=111111111&_pii=S0377042716303910&_rdoc=1&_issn=03770427&md5=0db60c1dda28e808aa115f522e3fb861" title="Click to view the MathML source">δ₃class="mathContainer hidden">class="mathCode"><math altimg="si77.gif" overflow="scroll"><msub><mrow><mi>δmi>mrow><mrow><mn>3mn>mrow>msub>math> and boundary discretization which is reported in the paper, clearly. In this article an appropriate constant mmlsi80" class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303910&_mathId=si80.gif&_user=111111111&_pii=S0377042716303910&_rdoc=1&_issn=03770427&md5=f37b798a400b11188603c30866113b35" title="Click to view the MathML source">c₀class="mathContainer hidden">class="mathCode"><math altimg="si80.gif" overflow="scroll"><msub><mrow><mi>cmi>mrow><mrow><mn>0mn>mrow>msub>math> is found which ensures uniqueness of solution of BIE with logarithmic kernel mmlsi81" class="mathmlsrc">class="formulatext stixSupport mathImg" data-mathURL="/science?_ob=MathURL&_method=retrieve&_eid=1-s2.0-S0377042716303910&_mathId=si81.gif&_user=111111111&_pii=S0377042716303910&_rdoc=1&_issn=03770427&md5=45418c9f61e6fac2691cd1b4fdc9d20f" title="Click to view the MathML source">ln(c₀r)class="mathContainer hidden">class="mathCode"><math altimg="si81.gif" overflow="scroll"><mo>lnmo><mrow><mo>(mo><msub><mrow><mi>cmi>mrow><mrow><mn>0mn>mrow>msub><mi>rmi><mo>)mo>mrow>math> as fundamental solution of Laplace equation. As a result, an upper bound for condition number of constant Galerkin BEMs system matrix is obtained when the size of boundary cells decreases. The upper bound found depends on three important issues: geometry of boundary, size of boundary cells and the kernel function. Also non-singular BIEs are proposed which can be used in boundary elements method (BEM) instead of singular ones to solve partial differential equations (PDEs). Then singular boundary integrals are vanished from BEM when the non-singular BIEs are used. Finally some numerical examples are presented which confirm the analytical results.