jscaux/pqed_html
1
0
Fork 0
Code Issues Pull Requests Releases Wiki Activity

Update 2022-03-24 08:43

Browse Source
This commit is contained in:
Jean-Sébastien
2022-03-24 08:43:21 +01:00
parent 1d852e7213
commit 50704eba07
211 changed files with 1506 additions and 3143 deletions
Download Patch File Download Diff File Expand all files Collapse all files
build/red_rm_Mf.html
+12 -12
View File
@@ -1,7 +1,7 @@
<!DOCTYPE html>
<html lang="en">
<head>
<!-- 2022-03-22 Tue 10:52 -->
<!-- 2022-03-24 Thu 08:42 -->
<meta charset="utf-8">
<meta name="viewport" content="width=device-width, initial-scale=1">
<title>Pre-Quantum Electrodynamics</title>
@@ -1293,7 +1293,7 @@ Table of contents
</summary>
<ul>
<li>
<a href="./qed_t.html#qed_t">QED today</a><span class="headline-id">qed.t</span>
<a href="./qed_L.html#qed_L">Lagrangian</a><span class="headline-id">qed.L</span>
</li>
@@ -1616,7 +1616,7 @@ Table of contents
<p>
Newton's second law remains valid provided we use the relativistic momentum:
</p>
<div class="core div" id="org11c93db">
<div class="core div" id="orge52f1a4">
<p>
<b>Newton's law</b> <i>(relativistic case)</i>
\[
@@ -1626,7 +1626,7 @@ Newton's second law remains valid provided we use the relativistic momentum:
</div>
<div class="example div" id="org4050d88">
<div class="example div" id="orgab74cfb">
<p>
<b>Example: motion under a constant force</b>
</p>
@@ -1657,7 +1657,7 @@ The particle's world line thus shows <b>hyperbolic motion</b>.
</p>
<figure id="orgd090155">
<figure id="org9244ff3">
<object type="image/svg+xml" data="./fig/red/red_motion_under_cst_F.svg" class="org-svg" alt="Relativistic motion under constant force">
Sorry, your browser does not support SVG.</object>
@@ -1726,15 +1726,15 @@ whereas the longitudinal component transforms in a complicated way:
For the specific case where the particle is instantaneously at rest in
the original frame, then
</p>
<div class="main div" id="org7c7f004">
<div class="eqlabel" id="org37e2037">
<div class="main div" id="orge9d30a6">
<div class="eqlabel" id="orga8b151c">
<p>
<a id="Ftr0"></a><a href="./red_rm_Mf.html#Ftr0"><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="orgbf7064d">
<div class="alteqlabels" id="org970f232">
</div>
@@ -1755,18 +1755,18 @@ The way to avoid complicated transformation rules is to define a four-vector
as the derivative of momentum with respect to proper time, which leads to
the definition of the
</p>
<div class="main div" id="orgc529917">
<div class="main div" id="org8fbba89">
<p>
<b>Minkowski force</b>
</p>
<div class="eqlabel" id="org24e429b">
<div class="eqlabel" id="orgd8fe9be">
<p>
<a id="MinkF"></a><a href="./red_rm_Mf.html#MinkF"><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="org6498650">
<div class="alteqlabels" id="orgcd1fb1c">
</div>
@@ -1806,7 +1806,7 @@ 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: 2022-03-22 Tue 10:52</p>
<p class="date">Created: 2022-03-24 Thu 08:42</p>
<p class="validation"></p>
</div>