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JSchoeberl committed Mar 18, 2024
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2 changes: 2 additions & 0 deletions _sources/sobolevspaces/Traces.ipynb
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"The interfaces are $\\gamma_{ij} = \\overline \\Omega_i \\cap \\overline \\Omega_j$.\n",
"The outer normal vector of $\\Omega_i$ is $n_i$.\n",
"\n",
"<img src=\"domaindecomposition.png\" alt=\"Alternative text\" width=\"250\" align=\"center\"/>\n",
"\n",
"> **Theorem:**\n",
"> Let $u \\in L_2(\\Omega)$ such that\n",
"> * $u_i := u|_{\\Omega_i}$ is in $H^1(\\Omega_i)$, and $g_i = \\nabla u_i$ is its\n",
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2 changes: 1 addition & 1 deletion searchindex.js

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11 changes: 6 additions & 5 deletions sobolevspaces/Traces.html
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<li class="toctree-l1 current active"><a class="current reference internal" href="#">15. Trace theorems and their applications</a></li>
<li class="toctree-l1"><a class="reference internal" href="equivalentnorms.html">16. Equivalent norms on <span class="math notranslate nohighlight">\(H^1\)</span> and on sub-spaces</a></li>
<li class="toctree-l1"><a class="reference internal" href="preciseweak.html">17. The weak formulation of the Poisson equation</a></li>
<li class="toctree-l1"><a class="reference internal" href="experiments.html">18. Experiments with norms (WIP)</a></li>
<li class="toctree-l1"><a class="reference internal" href="experiments.html">18. Experiments with norms</a></li>
<li class="toctree-l1"><a class="reference internal" href="exercises.html">19. Exercises</a></li>
</ul>
<p aria-level="2" class="caption" role="heading"><span class="caption-text">Finite Element Method</span></p>
Expand Down Expand Up @@ -675,6 +675,7 @@ <h2><span class="section-number">15.2. </span>Sobolev spaces over sub-domains<a
</ul>
<p>The interfaces are <span class="math notranslate nohighlight">\(\gamma_{ij} = \overline \Omega_i \cap \overline \Omega_j\)</span>.
The outer normal vector of <span class="math notranslate nohighlight">\(\Omega_i\)</span> is <span class="math notranslate nohighlight">\(n_i\)</span>.</p>
<a class="reference internal image-reference" href="../_images/domaindecomposition.png"><img alt="Alternative text" class="align-center" src="../_images/domaindecomposition.png" style="width: 250px;" /></a>
<blockquote>
<div><p><strong>Theorem:</strong>
Let <span class="math notranslate nohighlight">\(u \in L_2(\Omega)\)</span> such that</p>
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\]</div>
<p>Define the domain <span class="math notranslate nohighlight">\(\widetilde \Omega = \Omega \cup S_1 \cup \ldots \cup S_M\)</span>.</p>
<p>We define the extension operator by</p>
<div class="amsmath math notranslate nohighlight" id="equation-db688cc6-56eb-421c-980a-3f3724546b80">
<span class="eqno">()<a class="headerlink" href="#equation-db688cc6-56eb-421c-980a-3f3724546b80" title="Permalink to this equation">#</a></span>\[\begin{equation}
<div class="amsmath math notranslate nohighlight" id="equation-6f205c09-6ef5-4f39-ad24-b8cb50bbc7bb">
<span class="eqno">()<a class="headerlink" href="#equation-6f205c09-6ef5-4f39-ad24-b8cb50bbc7bb" title="Permalink to this equation">#</a></span>\[\begin{equation}
\begin{array}{rcll}
(E u) (\hat x) &amp; = &amp; u(x) &amp; \qquad \forall \, x \in \cup S_i \\
(Eu) (x) &amp; = &amp; u(x) &amp; \qquad \forall \, x \in \Omega
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\]</div>
<p>By definition of the weak derivative, there holds <span class="math notranslate nohighlight">\((z_k^\prime)^\prime = (1-\lambda_k) z_k\)</span>, i.e., <span class="math notranslate nohighlight">\(z^k \in H^2\)</span>. Since <span class="math notranslate nohighlight">\(H^2 \subset C^0\)</span>, there holds also
<span class="math notranslate nohighlight">\(z \in C^2\)</span>, and a weak solution is also a solution of the strong form</p>
<div class="amsmath math notranslate nohighlight" id="equation-d4c7c393-7e43-4018-abf4-2b99875187d1">
<span class="eqno">()<a class="headerlink" href="#equation-d4c7c393-7e43-4018-abf4-2b99875187d1" title="Permalink to this equation">#</a></span>\[\begin{equation}
<div class="amsmath math notranslate nohighlight" id="equation-ade41b7a-a0b7-4956-8dca-8de5868fa5df">
<span class="eqno">()<a class="headerlink" href="#equation-ade41b7a-a0b7-4956-8dca-8de5868fa5df" title="Permalink to this equation">#</a></span>\[\begin{equation}
\begin{array}{rcll}
z_k - z_k^{\prime \prime} &amp; = &amp; \lambda_k z_k \qquad &amp; \mbox{ on } (0,1) \\
z_k^\prime(0) = z_k^\prime(1) &amp; = &amp; 0
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