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Update 2022-03-15 10:07

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Jean-Sébastien
2022-03-15 10:07:27 +01:00
parent 4808df71e6
commit 55f0de8197
193 changed files with 2416 additions and 2082 deletions
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build/emsm_msm_lnlm_sp.html
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@@ -1,7 +1,7 @@
<!DOCTYPE html>
<html lang="en">
<head>
<!-- 2022-03-07 Mon 20:38 -->
<!-- 2022-03-15 Tue 08:10 -->
<meta charset="utf-8">
<meta name="viewport" content="width=device-width, initial-scale=1">
<title>Pre-Quantum Electrodynamics</title>
@@ -1310,10 +1310,6 @@ Table of contents
</summary>
<ul>
<li>
<a href="./d_m.html#d_m">Diagnostics: Mathematical Preliminaries</a><span class="headline-id">d.m</span>
</li>
<li>
<a href="./d_ems.html#d_ems">Diagnostics: Electromagnetostatics</a><span class="headline-id">d.ems</span>
</li>
@@ -1352,6 +1348,10 @@ Table of contents
<li>
<a href="./d_red.html#d_red">Diagnostics: Relativistic Electrodynamics</a><span class="headline-id">d.red</span>
</li>
<li>
<a href="./d_m.html#d_m">Diagnostics: Compendium - Mathematics</a><span class="headline-id">d.m</span>
</li>
</ul>
@@ -1618,15 +1618,15 @@ In para/diamagnets: when \({\bf B}\) is removed, \({\bf M}\) disappears. For n
fields, proportionality. Custom (slightly different than for dielectrics):
<b>magnetic susceptibility</b> \(\chi_m\) defined as
</p>
<div class="core div" id="orgf4940e6">
<div class="eqlabel" id="orgb9ff2cb">
<div class="core div" id="org690f8cb">
<div class="eqlabel" id="org530a5bc">
<p>
<a id="chim"></a><a href="./emsm_msm_lnlm_sp.html#chim"><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="org9c4be1d">
<div class="alteqlabels" id="org9587edf">
<ul class="org-ul">
<li>Gr (6.29)</li>
</ul>
@@ -1646,14 +1646,14 @@ fields, proportionality. Custom (slightly different than for dielectrics):
(and <b>not</b> \({\bf M} = \frac{1}{\mu_0} \chi_m {\bf B}\) had the electrostatics parallel
been followed historically). Materials that obey this are called <i>linear media</i>. Then,
</p>
<div class="eqlabel" id="org0da5e5c">
<div class="eqlabel" id="org92427e8">
<p>
<a id="BHM"></a><a href="./emsm_msm_lnlm_sp.html#BHM"><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="org5fb9aef">
<div class="alteqlabels" id="org93c272c">
<ul class="org-ul">
<li>Gr (6.30)</li>
</ul>
@@ -1668,14 +1668,14 @@ been followed historically). Materials that obey this are called <i>linear medi
\]
and thus
</p>
<div class="eqlabel" id="org4ced120">
<div class="eqlabel" id="org75fad04">
<p>
<a id="BH"></a><a href="./emsm_msm_lnlm_sp.html#BH"><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="orgaa26478">
<div class="alteqlabels" id="orgff9b371">
<ul class="org-ul">
<li>Gr (6.31)</li>
</ul>
@@ -1700,14 +1700,14 @@ have nonzero divergence.
<p>
In linear medium: bound volume current proportional to free current,
</p>
<div class="eqlabel" id="org06bf497">
<div class="eqlabel" id="org6b477dd">
<p>
<a id="JbchimJf"></a><a href="./emsm_msm_lnlm_sp.html#JbchimJf"><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="orge24d8e9">
<div class="alteqlabels" id="orge73774d">
<ul class="org-ul">
<li>Gr (6.33)</li>
</ul>
@@ -1742,7 +1742,7 @@ 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: 2022-03-07 Mon 20:38</p>
<p class="date">Created: 2022-03-15 Tue 08:10</p>
<p class="validation"></p>
</div>