Update 2022-02-14 06:33

This commit is contained in:
Jean-Sébastien
2022-02-14 06:33:37 +01:00
parent f8446c1405
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204 changed files with 1839 additions and 941 deletions
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<title>Pre-Quantum Electrodynamics</title>
@@ -1621,7 +1621,7 @@ We thus obtain
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Recognizing the proper velocity, we thus get that charge density and current density can together form the
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{\bf Current density 4-vector}
\[
@@ -1634,7 +1634,7 @@ Recognizing the proper velocity, we thus get that charge density and current den
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The continuity equation (\ref{eq:continuity}) takes the simple form
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{\bf Continuity equation}
\[
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while similarly the notation simplifies for
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{\bf Maxwell's equations}
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In terms of \(F^{\mu \nu}\) and the proper velocity \(\eta^\mu\), we also have the
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{\bf Minkowski force on a charge \(q\)}
\[
@@ -1711,7 +1711,7 @@ the Lorenz gauge (\ref{eq:InhomogeneousMaxwellLorenzGauge}) here expressed as
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Defining the
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{\bf d'Alembertian operator}
\[
@@ -1724,7 +1724,7 @@ Defining the
we obtain the final form of
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{\bf Maxwell's equations (Lorenz gauge, 4-vector notation)}
\[
@@ -1741,6 +1741,8 @@ of these equations.
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<br><ul class="navigation-links"><li>Prev:&nbsp;<a href="red_rem_Fmunu.html">The Field Tensor&emsp;<small>[red.rem.Fmunu]</small></a></li><li>Next:&nbsp;<a href="qed.html">Quantum Electrodynamics&emsp;<small>[qed]</small></a></li><li>Up:&nbsp;<a href="red_rem.html">Relativistic Electromagnetism&emsp;<small>[red.rem]</small></a></li></ul>
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<div class="license">
<a rel="license noopener" href="https://creativecommons.org/licenses/by/4.0/"
@@ -1754,7 +1756,7 @@ target="_blank">Creative Commons Attribution 4.0 International License</a>.
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<div id="postamble" class="status">
<p class="author">Author: Jean-Sébastien Caux</p>
<p class="date">Created: 2022-02-10 Thu 08:32</p>
<p class="date">Created: 2022-02-13 Sun 21:20</p>
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