Update 2022-02-09 22:41
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-02-09 Wed 07:31 -->
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<!-- 2022-02-09 Wed 22:40 -->
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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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@@ -408,17 +408,13 @@ Table of contents
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<li>
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<a href="./ems_es_ep_fp.html#ems_es_ep_fp">Field in terms of the potential</a><span class="headline-id">ems.es.ep.fp</span>
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</li>
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<li>
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<a href="./ems_es_ep_c.html#ems_es_ep_c">Comments on the Electrostatic Potential</a><span class="headline-id">ems.es.ep.c</span>
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</li>
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<li>
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<a href="./ems_es_ep_ex.html#ems_es_ep_ex">Example calculations for the potential</a><span class="headline-id">ems.es.ep.ex</span>
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</li>
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<li>
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<a href="./ems_es_ep_PL.html#ems_es_ep_PL">The Poisson Equation and the Laplace Equation</a><span class="headline-id">ems.es.ep.PL</span>
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<a href="./ems_es_ep_PL.html#ems_es_ep_PL">Poisson's and Laplace's Equations</a><span class="headline-id">ems.es.ep.PL</span>
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</li>
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<li>
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@@ -430,29 +426,8 @@ Table of contents
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</details>
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</li>
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<li>
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<details>
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<summary>
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<a href="./ems_es_e.html#ems_es_e">Electrostatic Energy from the Potential</a><span class="headline-id">ems.es.e</span>
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</summary>
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<ul>
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<li>
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<a href="./ems_es_e_pcd.html#ems_es_e_pcd">The Energy of a Point Charge Distribution</a><span class="headline-id">ems.es.e.pcd</span>
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</li>
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<li>
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<a href="./ems_es_e_ccd.html#ems_es_e_ccd">The Energy of a Continuous Charge Distribution</a><span class="headline-id">ems.es.e.ccd</span>
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</li>
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<li>
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<a href="./ems_es_e_c.html#ems_es_e_c">Comments on Electrostatic Energy</a><span class="headline-id">ems.es.e.c</span>
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</li>
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</ul>
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</details>
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</li>
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<li>
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@@ -1691,7 +1666,7 @@ so we get
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Substituting this in \ref{Gr(8.6)} and using the divergence theorem,
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we obtain
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</p>
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<div class="main div" id="org75886ff">
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<div class="main div" id="orgc3e7fad">
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<p>
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{\bf Poynting's theorem}
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\[
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@@ -1716,7 +1691,7 @@ energy is carried by EM fields out of \({\cal V}\) across its boundary surface.
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<p>
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Energy per unit time, per unit area carried by EM fields:
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</p>
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<div class="core div" id="orgb6d912b">
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<div class="core div" id="orgf0750fa">
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<p>
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{\bf Poynting vector}
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\[
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@@ -1729,7 +1704,7 @@ Energy per unit time, per unit area carried by EM fields:
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<p>
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We can thus express Poynting's theorem more compactly:
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</p>
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<div class="core div" id="org7131f77">
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<div class="core div" id="orged7fe8f">
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<p>
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{\bf Poynting's theorem}
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\[
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@@ -1742,7 +1717,7 @@ We can thus express Poynting's theorem more compactly:
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<p>
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where we have defined the total
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</p>
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<div class="core div" id="org44b728f">
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<div class="core div" id="org27d8494">
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<p>
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{\bf Energy in electromagnetic fields}
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\[
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@@ -1765,7 +1740,7 @@ Then,
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\]
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so we get the
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</p>
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<div class="core div" id="org11d0bdb">
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<div class="core div" id="org40d56f8">
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<p>
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{\bf Poynting theorem (differential form)}
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\[
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@@ -1782,7 +1757,7 @@ and has a similar for to the continuity equation
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<div class="example div" id="orgd2f58ae">
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<div class="example div" id="orge1eb64c">
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<p>
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\paragraph{Example 8.1} Current in a wire: Joule heating. Energy per unit time delivered to wire: from Poynting.
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Assuming that the field is uniform, the electric field parallel to the wire is
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@@ -1825,7 +1800,7 @@ 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: 2022-02-09 Wed 07:31</p>
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<p class="date">Created: 2022-02-09 Wed 22:40</p>
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<p class="validation"></p>
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</div>
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