Update 2022-03-24 08:43
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Jean-Sébastien
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@@ -1,7 +1,7 @@
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-03-22 Tue 10:52 -->
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<!-- 2022-03-24 Thu 08:42 -->
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<meta charset="utf-8">
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<meta name="viewport" content="width=device-width, initial-scale=1">
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<title>Pre-Quantum Electrodynamics</title>
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@@ -1293,7 +1293,7 @@ Table of contents
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</summary>
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<ul>
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<li>
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<a href="./qed_t.html#qed_t">QED today</a><span class="headline-id">qed.t</span>
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<a href="./qed_L.html#qed_L">Lagrangian</a><span class="headline-id">qed.L</span>
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</li>
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@@ -1617,14 +1617,14 @@ Table of contents
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In homogeneous linear dielectric, the bound charge density is directly
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proportional to the free charge:
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</p>
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<div class="eqlabel" id="org5a60e41">
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<div class="eqlabel" id="org3b1faf3">
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<p>
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<a id="rhob_ld"></a><a href="./emsm_esm_ld_bvp.html#rhob_ld"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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</svg></a>
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</p>
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<div class="alteqlabels" id="orgf2e150e">
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<div class="alteqlabels" id="org1fe40e5">
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<ul class="org-ul">
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<li>Gr (4.39)</li>
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</ul>
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@@ -1646,15 +1646,15 @@ and the potential then obeys the Laplace equation.
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It is convenient to rewrite our boundary conditions in terms of free charge densities:
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from <a href="./emsm_esm_D_bc.html#Dperp_disc">Dperp_disc</a>,
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</p>
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<div class="main div" id="orgf7ac2ac">
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<div class="eqlabel" id="org15ad919">
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<div class="main div" id="org1043649">
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<div class="eqlabel" id="org768d5d8">
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<p>
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<a id="Edisc_f"></a><a href="./emsm_esm_ld_bvp.html#Edisc_f"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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</svg></a>
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</p>
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<div class="alteqlabels" id="org2eadaf5">
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<div class="alteqlabels" id="orgb833c08">
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<ul class="org-ul">
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<li>Gr (4.40)</li>
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</ul>
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@@ -1673,15 +1673,15 @@ from <a href="./emsm_esm_D_bc.html#Dperp_disc">Dperp_disc</a>,
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<p>
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or in terms of the potential,
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</p>
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<div class="main div" id="org6b3545e">
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<div class="eqlabel" id="org2ef4740">
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<div class="main div" id="orgd7fd379">
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<div class="eqlabel" id="orgcd8da1d">
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<p>
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<a id="dpdisc_f"></a><a href="./emsm_esm_ld_bvp.html#dpdisc_f"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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</svg></a>
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</p>
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<div class="alteqlabels" id="orgd5ad929">
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<div class="alteqlabels" id="org49e04f7">
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<ul class="org-ul">
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<li>Gr (4.41)</li>
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</ul>
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@@ -1701,15 +1701,15 @@ or in terms of the potential,
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<p>
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The potential itself is continuous,
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</p>
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<div class="main div" id="org3ca662e">
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<div class="eqlabel" id="org833e744">
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<div class="main div" id="orged360ff">
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<div class="eqlabel" id="orgee30116">
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<p>
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<a id="pcont"></a><a href="./emsm_esm_ld_bvp.html#pcont"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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</svg></a>
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</p>
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<div class="alteqlabels" id="org27d0122">
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<div class="alteqlabels" id="orgb06a000">
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<ul class="org-ul">
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<li>Gr (4.42)</li>
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</ul>
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@@ -1727,7 +1727,7 @@ The potential itself is continuous,
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</div>
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<div class="example div" id="org34078f8">
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<div class="example div" id="org9c5f579">
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<p>
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<b>Example: sphere of homogeneous dielectric material in uniform electric field</b>
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</p>
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@@ -1794,7 +1794,7 @@ Thus,
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</div>
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<div class="example div" id="orgbbf1e7e">
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<div class="example div" id="org8809f63">
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<p>
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<b>Example: point charge above dielectric plane</b>
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</p>
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@@ -1876,7 +1876,7 @@ target="_blank">Creative Commons Attribution 4.0 International License</a>.
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</div>
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<div id="postamble" class="status">
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<p class="author">Author: Jean-Sébastien Caux</p>
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<p class="date">Created: 2022-03-22 Tue 10:52</p>
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<p class="date">Created: 2022-03-24 Thu 08:42</p>
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<p class="validation"></p>
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</div>
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