Update 2022-02-08 17:21

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Jean-Sébastien
2022-02-08 17:21:33 +01:00
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<title>Pre-Quantum Electrodynamics</title>
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<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>
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</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>
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<p>
Newton's second law remains valid provided we use the relativistic momentum:
</p>
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<p>
{\bf Newton's law (relativistic case)}
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<p>
\paragraph{Example 12.10: Motion under a constant force.} A particle
of mass \(m\) is subjected to a constant force \(F\). If it starts at the
@@ -1722,7 +1726,7 @@ 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
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{\bf Minkowski force}
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<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>
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