{"id":456,"date":"2017-11-23T05:41:44","date_gmt":"2017-11-23T05:41:44","guid":{"rendered":"https:\/\/blog.vanabel.cn\/?p=456"},"modified":"2017-11-23T06:16:00","modified_gmt":"2017-11-23T06:16:00","slug":"neumanbianzhiyudirichletbianzhidefansheyantuo","status":"publish","type":"post","link":"https:\/\/blog.vanabel.cn\/?p=456","title":{"rendered":"Neuman\u8fb9\u503c\u4e0eDirichlet\u8fb9\u503c\u7684\u53cd\u5c04\u5ef6\u62d3"},"content":{"rendered":"<p>\u6211\u4eec\u8003\u8651\u4e0a\u534a\u5706\u76d8$D$\u4e0a\u6700\u7b80\u5355\u7684Laplace\u65b9\u7a0b:<br \/>\n\\begin{equation}\\label{eq:n}<br \/>\n\\begin{cases}<br \/>\n\\Delta u=f\\in L^2(D),&#038;x\\in D\\\\<br \/>\n\\frac{\\partial u}{\\partial \\nu}=0,&#038;x\\in\\partial D<br \/>\n\\end{cases}<br \/>\n\\end{equation}<br \/>\n\u4e0e<br \/>\n\\begin{equation}\\label{eq:d}<br \/>\n\\begin{cases}<br \/>\n\\Delta u=f\\in L^2(D),&#038;x\\in D\\\\<br \/>\nu=0,&#038;x\\in\\partial D.<br \/>\n\\end{cases}<br \/>\n\\end{equation}<br \/>\n<div class='latex_thm'><span class='latex_thm_h'>\u5b9a\u7406 1<\/span><span class='latex_thm_h'>.<\/span> \u82e5\u6211\u4eec\u5bf9\\eqref{eq:n}, \u4f5c\u5076\u5ef6\u62d3$w(x)=\\begin{cases}u(x),&#038;x\\in D\\\\ u(x^*),&#038;x\\in D^-\\end{cases}$; \u5bf9\\eqref{eq:d}\u4f5c\u5947\u5ef6\u62d3$w(x)=\\begin{cases}u(x),&#038;x\\in D\\\\-u(x^*),&#038;x\\in D^-\\end{cases}$. \u5219\u53ef\u9a8c\u8bc1, \u5ef6\u62d3\u540e\u7684$w$\u662f\u65b9\u7a0b\\eqref{eq:d}\u5728$B=D\\cup D^-$\u4e0a\u7684$W^{1,2}$\u5f31\u89e3\u3002<br \/>\n<\/div><br \/>\n<!--more--><\/p>\n<p>\u4e8b\u5b9e\u4e0a, \u5bf9\\eqref{eq:n}\u53ea\u9700\u9a8c\u8bc1, \u5bf9$\\varphi\\in  C^\\infty(B)$, \u6210\u7acb<br \/>\n\\begin{equation}\\label{eq:wn}<br \/>\n\\int_B\\nabla w\\nabla\\varphi+w\\varphi=0.<br \/>\n\\end{equation}<br \/>\n\u800c\u5bf9\\eqref{eq:d}\u53ea\u9700\u9a8c\u8bc1, \u5bf9$\\varphi\\in C_0^\\infty(B)$, \u6210\u7acb<br \/>\n\\begin{equation}\\label{eq:wd}<br \/>\n\\int_B\\nabla w\\nabla\\varphi+w\\varphi=0.<br \/>\n\\end{equation}<br \/>\n\u9996\u5148, \u5bf9\\eqref{eq:n}\u7684\u89e3\u6765\u9a8c\u8bc1\u3002\u5bf9$\\varphi\\in  C^\\infty(B)$, \u4ee4<br \/>\n$$<br \/>\n\\varphi_e=\\frac{1}{2}(\\varphi(x)+\\varphi(x^*)),\\quad<br \/>\n\\varphi_o=\\frac{1}{2}(\\varphi(x)-\\varphi(x^*))<br \/>\n$$<br \/>\n\u5206\u522b\u4e3a\u5176\u5076\u90e8\u5206\u4e0e\u5947\u90e8\u5206\u3002\u76f4\u63a5\u8ba1\u7b97\u5f97\u5230\uff1a<br \/>\n\\begin{align*}<br \/>\n\\int_B\\nabla w\\nabla\\varphi+w\\varphi&#038;=\\int_B\\nabla w\\nabla\\varphi_e+w\\varphi_e+<br \/>\n\\int_B\\nabla w\\nabla\\varphi_o+w\\varphi_o\\\\<br \/>\n\\int_B\\nabla w\\nabla\\varphi_e+w\\varphi_e&#038;=\\int_D\\nabla u\\nabla\\varphi_e+u\\varphi_e+\\int_{D^-}\\nabla u(x^*)\\nabla\\varphi_e+u(x^*)\\varphi_e\\\\<br \/>\n\\int_{D^-}\\nabla u(x^*)\\nabla\\varphi_e+u(x^*)\\varphi_edx&#038;=\\int_{D}\\nabla u\\nabla\\varphi_e(x^*)+u\\varphi_e(x^*)\\\\<br \/>\n&#038;=\\int_D\\nabla u\\nabla\\varphi_e+u\\varphi_e\\\\<br \/>\n\\int_B\\nabla w\\nabla\\varphi_o+w\\varphi_o&#038;=\\int_D\\nabla w\\nabla\\varphi_o+w\\varphi_o+\\int_{D^-}\\nabla w\\nabla\\varphi_o+w\\varphi_o\\\\<br \/>\n&#038;=\\int_D\\nabla u\\nabla\\varphi_o+u\\varphi_o+\\int_{D^-}\\nabla u(x^*)\\nabla\\varphi_o+u(x^*)\\varphi_o\\\\<br \/>\n\\int_{D^-}\\nabla u(x^*)\\nabla\\varphi_o+u(x^*)\\varphi_o&#038;=\\int_D\\nabla u\\nabla\\varphi_o(x^*)+u\\varphi_o(x^*)\\\\<br \/>\n&#038;=-\\int_D\\nabla u\\nabla\\varphi_o+u\\varphi_o<br \/>\n\\end{align*}<br \/>\n\u7531\u4e8e$\\varphi\\in C^\\infty(B)$\u6545$\\varphi_e\\in C^\\infty(D)$. \u800c$u$\u662f\\eqref{eq:n}\u5728$D$\u4e0a\u7684$W^{1,2}$\u5f31\u89e3, \u4e8e\u662f<br \/>\n$$<br \/>\n\\int_D\\nabla u\\nabla\\varphi_e+u\\varphi_e=0.<br \/>\n$$<br \/>\n\u8fd9\u6837, \u6211\u4eec\u5c31\u8bc1\u660e\u4e86<br \/>\n$$<br \/>\n\\int_B\\nabla w\\nabla\\varphi+w\\varphi=0,\\quad\\varphi\\in C^\\infty(B).<br \/>\n$$<\/p>\n<p>\u5bf9\\eqref{eq:d}\u7684\u89e3\u7684\u9a8c\u8bc1\u662f\u7c7b\u4f3c\u7684. \u53ea\u9700\u6ce8\u610f\u5230, \u5bf9$\\varphi=\\varphi_e+\\varphi_o\\in C_0^\\infty(B)$, \u548c\u524d\u9762\u5bf9Neumann\u60c5\u5f62\u7684\u9a8c\u8bc1\u4e00\u6837, \u6211\u4eec\u4ecd\u7136\u53ef\u4ee5\u5f97\u5230(\u6ce8\u610f\u6b64\u65f6$w$\u662f\u5947\u5ef6\u62d3),<br \/>\n\\begin{align*}<br \/>\n\\int_B\\nabla w\\nabla\\varphi+w\\varphi&#038;=\\int_B\\nabla w\\nabla\\varphi_e+w\\varphi_e+<br \/>\n\\int_B\\nabla w\\nabla\\varphi_o+w\\varphi_o\\\\<br \/>\n\\int_B\\nabla w\\nabla\\varphi_e+w\\varphi_e&#038;=\\int_D\\nabla u\\nabla\\varphi_e+u\\varphi_e\\color{red}{-}\\int_{D^-}\\nabla u(x^*)\\nabla\\varphi_e+u(x^*)\\varphi_e\\\\<br \/>\n&#038;=0\\\\<br \/>\n\\int_B\\nabla w\\nabla\\varphi_o+w\\varphi_o&#038;=\\int_D\\nabla w\\nabla\\varphi_o+w\\varphi_o+\\int_{D^-}\\nabla w\\nabla\\varphi_o+w\\varphi_o\\\\<br \/>\n&#038;=\\int_D\\nabla u\\nabla\\varphi_o+u\\varphi_o\\color{red}{-}\\int_{D^-}\\nabla u(x^*)\\nabla\\varphi_o+u(x^*)\\varphi_o\\\\<br \/>\n&#038;=2\\int_D\\nabla u\\nabla\\varphi_o+u\\varphi_o.<br \/>\n\\end{align*}<br \/>\n\u7531\u4e8e$\\varphi\\in C_0^\\infty(B)$, \u6211\u4eec\u77e5\u9053$\\varphi_o\\in C_0^\\infty(B)$\u4e14$\\varphi_o|_{\\partial^0D}=0$. \u8fd9\u91cc, $\\partial^0D=\\{x=(x^1,x^2)\\in D:x_2=0\\}$, $\\partial^+D=\\{x\\in\\partial D:x^2>0\\}$. \u56e0\u6b64, \u5b9e\u9645\u4e0a$\\varphi_o\\in C_0^\\infty(D)$. \u6545\u7531$u$\u662f\\eqref{eq:d}\u5728$D$\u4e0a\u7684\u5f31\u89e3\u77e5\u9053<br \/>\n$$<br \/>\n\\int_D\\nabla u\\nabla\\varphi_o+u\\varphi_o=0.<br \/>\n$$<br \/>\n\u8fd9\u6837, \u6211\u4eec\u5c31\u8bc1\u660e\u4e86<br \/>\n$$<br \/>\n\\int_B\\nabla w\\nabla\\varphi+w\\varphi=0,\\quad\\varphi\\in C_0^\\infty(B).<br \/>\n$$<\/p>\n","protected":false},"excerpt":{"rendered":"<p>\u6211\u4eec\u8003\u8651\u4e0a\u534a\u5706\u76d8$D$\u4e0a\u6700\u7b80\u5355\u7684Laplace\u65b9\u7a0b: \\begin{equation}\\label{eq:n}&hellip; <a class=\"more-link\" href=\"https:\/\/blog.vanabel.cn\/?p=456\">\u7ee7\u7eed\u9605\u8bfb<span class=\"screen-reader-text\">Neuman\u8fb9\u503c\u4e0eDirichlet\u8fb9\u503c\u7684\u53cd\u5c04\u5ef6\u62d3<\/span><\/a><\/p>\n","protected":false},"author":1,"featured_media":0,"comment_status":"open","ping_status":"open","sticky":false,"template":"","format":"standard","meta":{"footnotes":""},"categories":[2],"tags":[102,104,79,103],"class_list":["post-456","post","type-post","status-publish","format-standard","hentry","category-math","tag-pde","tag-yantuo","tag-ruojie","tag-bianzhi","entry"],"_links":{"self":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/456","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts"}],"about":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/types\/post"}],"author":[{"embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fcomments&post=456"}],"version-history":[{"count":5,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/456\/revisions"}],"predecessor-version":[{"id":461,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=\/wp\/v2\/posts\/456\/revisions\/461"}],"wp:attachment":[{"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fmedia&parent=456"}],"wp:term":[{"taxonomy":"category","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Fcategories&post=456"},{"taxonomy":"post_tag","embeddable":true,"href":"https:\/\/blog.vanabel.cn\/index.php?rest_route=%2Fwp%2Fv2%2Ftags&post=456"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}