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Update 2022-03-24 08:43

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Jean-Sébastien
2022-03-24 08:43:21 +01:00
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commit 50704eba07
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build/ems_es_ep_PL.html
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@@ -1,7 +1,7 @@
<!DOCTYPE html>
<html lang="en">
<head>
<!-- 2022-03-22 Tue 10:52 -->
<!-- 2022-03-24 Thu 08:42 -->
<meta charset="utf-8">
<meta name="viewport" content="width=device-width, initial-scale=1">
<title>Pre-Quantum Electrodynamics</title>
@@ -1293,7 +1293,7 @@ Table of contents
</summary>
<ul>
<li>
<a href="./qed_t.html#qed_t">QED today</a><span class="headline-id">qed.t</span>
<a href="./qed_L.html#qed_L">Lagrangian</a><span class="headline-id">qed.L</span>
</li>
@@ -1622,14 +1622,14 @@ Our two fundamental equations for the electrostatic field are
\]
For the electrostatic potential, by <a href="./ems_es_ep_fp.html#Emgp">Emgp</a>, Gauss's law becomes
</p>
<div class="eqlabel" id="orga248783">
<div class="eqlabel" id="org2b4e2eb">
<p>
<a id="Poi"></a><a href="./ems_es_ep_PL.html#Poi"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
<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"/>
<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"/>
</svg></a>
</p>
<div class="alteqlabels" id="org2e27297">
<div class="alteqlabels" id="orgfd2b954">
<ul class="org-ul">
<li>Gr (2.24)</li>
<li>PM (2.72)</li>
@@ -1638,7 +1638,7 @@ For the electrostatic potential, by <a href="./ems_es_ep_fp.html#Emgp">Emgp</a>,
</div>
</div>
<div class="core div" id="org2b5be1d">
<div class="core div" id="org36797b7">
<p>
<b>Poisson's equation</b>
\[
@@ -1651,14 +1651,14 @@ For the electrostatic potential, by <a href="./ems_es_ep_fp.html#Emgp">Emgp</a>,
<p>
When the charge density vanishes, it becomes more simply
</p>
<div class="eqlabel" id="org98e969b">
<div class="eqlabel" id="org97e70d7">
<p>
<a id="Lap"></a><a href="./ems_es_ep_PL.html#Lap"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
<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"/>
<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"/>
</svg></a>
</p>
<div class="alteqlabels" id="org1b9ea13">
<div class="alteqlabels" id="org5b0e4aa">
<ul class="org-ul">
<li>Gr (2.25)</li>
<li>PM (2.75)</li>
@@ -1667,7 +1667,7 @@ When the charge density vanishes, it becomes more simply
</div>
</div>
<div class="core div" id="orgdc0fc61">
<div class="core div" id="org2470271">
<p>
<b>Laplace's Equation</b>
\[
@@ -1703,7 +1703,7 @@ target="_blank">Creative Commons Attribution 4.0 International License</a>.
</div>
<div id="postamble" class="status">
<p class="author">Author: Jean-Sébastien Caux</p>
<p class="date">Created: 2022-03-22 Tue 10:52</p>
<p class="date">Created: 2022-03-24 Thu 08:42</p>
<p class="validation"></p>
</div>