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Update 2022-02-08 17:21

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Jean-Sébastien
2022-02-08 17:21:33 +01:00
parent 077433c40a
commit 3454aba504
207 changed files with 1882 additions and 1097 deletions
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build/ems_es_efo_e.html
+16 -6
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@@ -1,7 +1,7 @@
<!DOCTYPE html>
<html lang="en">
<head>
<!-- 2022-02-08 Tue 06:55 -->
<!-- 2022-02-08 Tue 17:21 -->
<meta charset="utf-8">
<meta name="viewport" content="width=device-width, initial-scale=1">
<title>Pre-Quantum Electrodynamics</title>
@@ -272,6 +272,10 @@ Table of contents
</summary>
<ul>
<li>
<a href="./in_t_l.html#in_t_l">Section and equation labelling</a><span class="headline-id">in.t.l</span>
</li>
<li>
<a href="./in_t_c.html#in_t_c">Contextual colors</a><span class="headline-id">in.t.c</span>
</li>
@@ -736,7 +740,7 @@ Table of contents
</li>
<li>
<a href="./emsm_esm_d.html#emsm_esm_d">Dielectrics</a><span class="headline-id">emsm.esm.d</span>
<a href="./emsm_esm_di.html#emsm_esm_di">Dielectrics</a><span class="headline-id">emsm.esm.di</span>
</li>
<li>
@@ -1661,8 +1665,14 @@ For the path, the 'angular' part is not contributing (see drawings in
FLS II 4-3). The integral is thus purely radial,
</p>
<div class="eqlabel" id="org70d5df1">
<div class="alteqlabels" id="org206a74a">
<div class="eqlabel" id="org34ece66">
<p>
<a id="Wab"></a><a href="./ems_es_efo_e.html#Wab"><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="org003f3b8">
<ul class="org-ul">
<li>Gr (2.18)</li>
</ul>
@@ -1673,7 +1683,7 @@ FLS II 4-3). The integral is thus purely radial,
\begin{equation}
-\int_{\bf a}^{\bf b} {\bf F} \cdot d{\bf l}
= -\frac{q_t q_s}{4\pi \varepsilon_0} \int_{r_a}^{r_b} \frac{dr}{r^2} = \frac{q_t q_s}{4\pi \varepsilon_0} \left(\frac{1}{r_b} - \frac{1}{r_a}\right).
\label{Gr(2.18)}
\tag{Wab}\label{Wab}
\end{equation}
<p>
@@ -1736,7 +1746,7 @@ where in the second equality we have symmetrized the sums for convenience.
<hr><div id="postamble" class="status">
<p class="author">Author: Jean-Sébastien Caux</p>
<p class="date">Created: 2022-02-08 Tue 06:55</p>
<p class="date">Created: 2022-02-08 Tue 17:21</p>
<p class="validation"><a href="https://validator.w3.org/check?uri=referer">Validate</a></p>
</div>