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Update 2022-02-10 08:34

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Jean-Sébastien
2022-02-10 08:34:34 +01:00
parent f3c2446d19
commit f8446c1405
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build/ems_es_c_p.html
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<!DOCTYPE html>
<html lang="en">
<head>
<!-- 2022-02-09 Wed 22:40 -->
<!-- 2022-02-10 Thu 08:32 -->
<meta charset="utf-8">
<meta name="viewport" content="width=device-width, initial-scale=1">
<title>Pre-Quantum Electrodynamics</title>
@@ -1597,7 +1597,7 @@ Table of contents
<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><span class="headline-id">ems.es.c.p</span></h5>
<div class="outline-text-5" id="text-ems_es_c_p">
<div class="main div" id="orgd8d7d4b">
<div class="main div" id="orgcfb8b0f">
<p>
<b>Basic Properties of a Conductor</b>
</p>
@@ -1610,14 +1610,10 @@ Table of contents
<b>(iii) Any net charge resides on the surface</b>.</li>
<li><b>(iv) A conductor is an equipotential.</b></li>
<li>
<b>(v)</b> \({\bf E}\) is perpendicular to the surface, just outside the conductor.}</li>
<b>(v)</b> \({\bf E}\) is perpendicular to the surface, just outside the conductor.</li>
</ul>
</div>
<p>
Note that (iv) links directly with our second case of solving Poisson's equation above:
for a system of conductors held at fixed potentials, the solution is unique.
</p>
</div>
</div>
@@ -1636,7 +1632,7 @@ 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: 2022-02-09 Wed 22:40</p>
<p class="date">Created: 2022-02-10 Thu 08:32</p>
<p class="validation"></p>
</div>