Update 2022-03-07 20:40
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-03-02 Wed 15:45 -->
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<!-- 2022-03-07 Mon 20:38 -->
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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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@@ -1098,14 +1098,6 @@ Table of contents
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<li>
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<a href="./emdm_emwm_refl_oi.html#emdm_emwm_refl_oi">Oblique Incidence</a><span class="headline-id">emdm.emwm.refl.oi</span>
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</li>
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<li>
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<a href="./emdm_emwm_refl_Fe.html#emdm_emwm_refl_Fe">Fresnel's Equations</a><span class="headline-id">emdm.emwm.refl.Fe</span>
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</li>
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<li>
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<a href="./emdm_emwm_refl_Ba.html#emdm_emwm_refl_Ba">Brewster's Angle</a><span class="headline-id">emdm.emwm.refl.Ba</span>
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</li>
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</ul>
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@@ -1691,7 +1683,7 @@ how the nonvanishing elements of an antisymmetric tensor transform:
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<p>
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Comparing with the transformation rules for the electromagnetic field which we obtained in (\ref{eq:EMFieldsLorentzTransfo}), we can define the
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</p>
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<div class="core div" id="orga4ad8ae">
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<div class="core div" id="orge72c66d">
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<p>
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{\bf Electromagnetic Field Tensor}
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\[
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@@ -1707,7 +1699,7 @@ Comparing with the transformation rules for the electromagnetic field which we o
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<p>
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together with the handy
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</p>
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<div class="main div" id="orge2eae7f">
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<div class="main div" id="org5c6516a">
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<p>
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{\bf Dual Field Tensor}
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\[
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@@ -1731,7 +1723,7 @@ obtained from the field tensor by the substitution
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<p>
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Our electromagnetic field transformation laws then become the simple
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</p>
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<div class="core div" id="org8271014">
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<div class="core div" id="org7f5ef81">
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<p>
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{\bf Lorentz Transformation Rules for EM Fields}
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\[
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@@ -1761,7 +1753,7 @@ 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: 2022-03-02 Wed 15:45</p>
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<p class="date">Created: 2022-03-07 Mon 20:38</p>
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<p class="validation"></p>
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</div>
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