Update 2022-03-07 20:40

This commit is contained in:
Jean-Sébastien
2022-03-07 20:40:36 +01:00
parent 21bf9fdba5
commit 4808df71e6
194 changed files with 1487 additions and 5980 deletions
+6 -14
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@@ -1,7 +1,7 @@
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<meta charset="utf-8">
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<title>Pre-Quantum Electrodynamics</title>
@@ -1098,14 +1098,6 @@ Table of contents
<li>
<a href="./emdm_emwm_refl_oi.html#emdm_emwm_refl_oi">Oblique Incidence</a><span class="headline-id">emdm.emwm.refl.oi</span>
</li>
<li>
<a href="./emdm_emwm_refl_Fe.html#emdm_emwm_refl_Fe">Fresnel's Equations</a><span class="headline-id">emdm.emwm.refl.Fe</span>
</li>
<li>
<a href="./emdm_emwm_refl_Ba.html#emdm_emwm_refl_Ba">Brewster's Angle</a><span class="headline-id">emdm.emwm.refl.Ba</span>
</li>
</ul>
@@ -1626,14 +1618,14 @@ For a conductor, we can exploit the fact that electrical fields vanish on the in
get a proper boundary condition for the potential. Namely, here, boundary condition
<a href="./ems_es_ep_bc.html#Edisc">Edisc</a> yields
</p>
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<div class="alteqlabels" id="org7b42f41">
<div class="alteqlabels" id="org6b2bac5">
<ul class="org-ul">
<li>Gr (2.48)</li>
</ul>
@@ -1651,14 +1643,14 @@ get a proper boundary condition for the potential. Namely, here, boundary condi
<p>
which in terms of potential reads
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<a id="scd_cond"></a><a href="./ems_es_c_sc.html#scd_cond"><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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<div class="alteqlabels" id="org1719e76">
<div class="alteqlabels" id="org57e15c0">
<ul class="org-ul">
<li>Gr (2.49)</li>
</ul>
@@ -1720,7 +1712,7 @@ 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: 2022-03-02 Wed 15:45</p>
<p class="date">Created: 2022-03-07 Mon 20:38</p>
<p class="validation"></p>
</div>