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>
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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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<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>
<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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@@ -1688,7 +1692,7 @@ how the nonvanishing elements of an antisymmetric tensor transform:
<p>
Comparing with the transformation rules for the electromagnetic field which we obtained in (\ref{eq:EMFieldsLorentzTransfo}), we can define the
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{\bf Electromagnetic Field Tensor}
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together with the handy
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{\bf Dual Field Tensor}
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<p>
Our electromagnetic field transformation laws then become the simple
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{\bf Lorentz Transformation Rules for EM Fields}
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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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