Update 2022-02-14 20:42
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-02-13 Sun 21:20 -->
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<!-- 2022-02-14 Mon 20:35 -->
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<meta charset="utf-8">
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<meta name="viewport" content="width=device-width, initial-scale=1">
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<title>Pre-Quantum Electrodynamics</title>
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@@ -1600,7 +1600,7 @@ Table of contents
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<p>
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Newton's second law remains valid provided we use the relativistic momentum:
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</p>
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<div class="core div" id="org3dd1bf3">
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<div class="core div" id="org93299b0">
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<p>
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{\bf Newton's law (relativistic case)}
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\[
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@@ -1610,7 +1610,7 @@ Newton's second law remains valid provided we use the relativistic momentum:
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</div>
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<div class="example div" id="orge3da9b6">
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<div class="example div" id="org2540972">
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<p>
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\paragraph{Example 12.10: Motion under a constant force.} A particle
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of mass \(m\) is subjected to a constant force \(F\). If it starts at the
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@@ -1701,7 +1701,7 @@ The way to avoid complicated transformation rules is to define a four-vector
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as the derivative of momentum with respect to proper time, which leads to
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the definition of the
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</p>
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<div class="main div" id="org60615d2">
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<div class="main div" id="orgfb38297">
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<p>
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{\bf Minkowski force}
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\[
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@@ -1738,7 +1738,7 @@ target="_blank">Creative Commons Attribution 4.0 International License</a>.
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</div>
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<div id="postamble" class="status">
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<p class="author">Author: Jean-Sébastien Caux</p>
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<p class="date">Created: 2022-02-13 Sun 21:20</p>
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<p class="date">Created: 2022-02-14 Mon 20:35</p>
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<p class="validation"></p>
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</div>
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