Update 2022-03-01 08:15

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Jean-Sébastien
2022-03-01 08:15:26 +01:00
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<!-- 2022-02-21 Mon 20:41 -->
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<meta charset="utf-8">
<meta name="viewport" content="width=device-width, initial-scale=1">
<title>Pre-Quantum Electrodynamics</title>
@@ -1645,7 +1645,7 @@ We thus obtain
\]
Recognizing the proper velocity, we thus get that charge density and current density can together form the
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<p>
{\bf Current density 4-vector}
\[
@@ -1658,7 +1658,7 @@ Recognizing the proper velocity, we thus get that charge density and current den
<p>
The continuity equation (\ref{eq:continuity}) takes the simple form
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{\bf Continuity equation}
\[
@@ -1670,7 +1670,7 @@ The continuity equation (\ref{eq:continuity}) takes the simple form
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while similarly the notation simplifies for
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<p>
{\bf Maxwell's equations}
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@@ -1685,7 +1685,7 @@ while similarly the notation simplifies for
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In terms of \(F^{\mu \nu}\) and the proper velocity \(\eta^\mu\), we also have the
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<p>
{\bf Minkowski force on a charge \(q\)}
\[
@@ -1735,7 +1735,7 @@ the Lorenz gauge (\ref{eq:InhomogeneousMaxwellLorenzGauge}) here expressed as
\]
Defining the
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{\bf d'Alembertian operator}
\[
@@ -1748,7 +1748,7 @@ Defining the
we obtain the final form of
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{\bf Maxwell's equations (Lorenz gauge, 4-vector notation)}
\[
@@ -1780,7 +1780,7 @@ target="_blank">Creative Commons Attribution 4.0 International License</a>.
</div>
<div id="postamble" class="status">
<p class="author">Author: Jean-Sébastien Caux</p>
<p class="date">Created: 2022-02-21 Mon 20:41</p>
<p class="date">Created: 2022-03-01 Tue 08:14</p>
<p class="validation"></p>
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