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Update 2022-02-14 06:33

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Jean-Sébastien
2022-02-14 06:33:37 +01:00
parent f8446c1405
commit 4cfe8cef59
204 changed files with 1839 additions and 941 deletions
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build/ems_es_ep_PL.html
+10 -8
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@@ -1,7 +1,7 @@
<!DOCTYPE html>
<html lang="en">
<head>
<!-- 2022-02-10 Thu 08:32 -->
<!-- 2022-02-13 Sun 21:20 -->
<meta charset="utf-8">
<meta name="viewport" content="width=device-width, initial-scale=1">
<title>Pre-Quantum Electrodynamics</title>
@@ -1606,14 +1606,14 @@ 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="orgc8206b6">
<div class="eqlabel" id="org46a7e08">
<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="org7f36fce">
<div class="alteqlabels" id="org5ba9c0d">
<ul class="org-ul">
<li>Gr (2.24)</li>
<li>PM (2.72)</li>
@@ -1622,7 +1622,7 @@ For the electrostatic potential, by <a href="./ems_es_ep_fp.html#Emgp">Emgp</a>,
</div>
</div>
<div class="core div" id="org6dc641b">
<div class="core div" id="org0474445">
<p>
<b>Poisson's equation</b>
\[
@@ -1635,14 +1635,14 @@ 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="org1c1da98">
<div class="eqlabel" id="orgd2d2d62">
<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="org9d6fd1b">
<div class="alteqlabels" id="org8fd85ec">
<ul class="org-ul">
<li>Gr (2.25)</li>
<li>PM (2.75)</li>
@@ -1651,7 +1651,7 @@ When the charge density vanishes, it becomes more simply
</div>
</div>
<div class="core div" id="org17ea801">
<div class="core div" id="org7c1ca13">
<p>
<b>Laplace's Equation</b>
\[
@@ -1672,6 +1672,8 @@ Since the curl of a gradient is always zero, we by construction have
<br><ul class="navigation-links"><li>Prev:&nbsp;<a href="ems_es_ep_ex.html">Example calculations for the potential&emsp;<small>[ems.es.ep.ex]</small></a></li><li>Next:&nbsp;<a href="ems_es_ep_bc.html">Electrostatic Boundary Conditions&emsp;<small>[ems.es.ep.bc]</small></a></li><li>Up:&nbsp;<a href="ems_es_ep.html">The Electrostatic Potential&emsp;<small>[ems.es.ep]</small></a></li></ul>
<br>
<hr>
<div class="license">
<a rel="license noopener" href="https://creativecommons.org/licenses/by/4.0/"
@@ -1685,7 +1687,7 @@ 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: 2022-02-10 Thu 08:32</p>
<p class="date">Created: 2022-02-13 Sun 21:20</p>
<p class="validation"></p>
</div>