Update 2022-02-08 17:21
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@@ -1,7 +1,7 @@
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-02-08 Tue 06:55 -->
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<!-- 2022-02-08 Tue 17:21 -->
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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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@@ -272,6 +272,10 @@ Table of contents
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</summary>
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<ul>
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<li>
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<a href="./in_t_l.html#in_t_l">Section and equation labelling</a><span class="headline-id">in.t.l</span>
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</li>
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<li>
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<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>
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@@ -736,7 +740,7 @@ Table of contents
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</li>
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<li>
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<a href="./emsm_esm_d.html#emsm_esm_d">Dielectrics</a><span class="headline-id">emsm.esm.d</span>
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<a href="./emsm_esm_di.html#emsm_esm_di">Dielectrics</a><span class="headline-id">emsm.esm.di</span>
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</li>
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<li>
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@@ -1633,7 +1637,7 @@ in which the first integral can be interpreted as the momentum stored in the EM
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<p>
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This is thus simply a conservation law for momentum, with
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</p>
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<div class="main div" id="org2bb42ec">
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<div class="main div" id="orgeb408ef">
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<p>
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{\bf Momentum density in the EM fields}
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\[
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@@ -1645,7 +1649,7 @@ This is thus simply a conservation law for momentum, with
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<p>
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In a region in which the mechanical momentum is not changing due to external influences, we then have the
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</p>
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<div class="main div" id="orgaafc4b4">
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<div class="main div" id="org94bfc0c">
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<p>
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{\bf Continuity equation for EM momentum}
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\[
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@@ -1661,7 +1665,7 @@ In a region in which the mechanical momentum is not changing due to external inf
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<hr><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: 2022-02-08 Tue 06:55</p>
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<p class="date">Created: 2022-02-08 Tue 17:21</p>
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<p class="validation"><a href="https://validator.w3.org/check?uri=referer">Validate</a></p>
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</div>
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