Update 2022-02-14 20:42
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@@ -1,7 +1,7 @@
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<!DOCTYPE html>
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<html lang="en">
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<head>
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<!-- 2022-02-13 Sun 21:20 -->
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<!-- 2022-02-14 Mon 20:35 -->
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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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@@ -1614,14 +1614,14 @@ In one dimension, the potential is a single-variable
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function \(\phi (x)\) and the Laplace equation reads
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</p>
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<div class="eqlabel" id="org8b9eaa8">
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<div class="eqlabel" id="org937348d">
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<p>
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<a id="Lap_1d"></a><a href="./ems_ca_fe_L.html#Lap_1d"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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</svg></a>
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</p>
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<div class="alteqlabels" id="org1a79944">
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<div class="alteqlabels" id="orgf7c0132">
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</div>
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@@ -1636,14 +1636,14 @@ function \(\phi (x)\) and the Laplace equation reads
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<p>
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The solution to this
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</p>
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<div class="eqlabel" id="orgd6d6f8b">
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<div class="eqlabel" id="org5437a41">
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<p>
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<a id="Lap_1d_sol"></a><a href="./ems_ca_fe_L.html#Lap_1d_sol"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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</svg></a>
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</p>
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<div class="alteqlabels" id="org135f906">
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<div class="alteqlabels" id="org777e948">
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<ul class="org-ul">
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<li>Gr (3.6)</li>
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</ul>
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@@ -1702,14 +1702,14 @@ In two dimensions, the potential becomes a function
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of two variables (here: \(x\) and \(y\)), so Laplace's
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equation now reads
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</p>
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<div class="eqlabel" id="orgb8aa28d">
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<div class="eqlabel" id="orgf26c98b">
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<p>
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<a id="Lap_2d"></a><a href="./ems_ca_fe_L.html#Lap_2d"><svg xmlns="http://www.w3.org/2000/svg" width="16" height="16" fill="currentColor" class="bi bi-link" viewBox="0 0 16 16">
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<path d="M6.354 5.5H4a3 3 0 0 0 0 6h3a3 3 0 0 0 2.83-4H9c-.086 0-.17.01-.25.031A2 2 0 0 1 7 10.5H4a2 2 0 1 1 0-4h1.535c.218-.376.495-.714.82-1z"/>
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<path d="M9 5.5a3 3 0 0 0-2.83 4h1.098A2 2 0 0 1 9 6.5h3a2 2 0 1 1 0 4h-1.535a4.02 4.02 0 0 1-.82 1H12a3 3 0 1 0 0-6H9z"/>
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</svg></a>
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</p>
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<div class="alteqlabels" id="org01054fc">
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<div class="alteqlabels" id="org59e7c1d">
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</div>
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@@ -1765,8 +1765,8 @@ a point equals its value averaged over any sphere
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\]
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</p>
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<details id="org8c78d21">
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<summary id="org6bdc443">
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<details id="orgf3cada4">
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<summary id="org840c868">
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<strong>Physicist's proof</strong>
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</summary>
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<p>
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@@ -1833,8 +1833,8 @@ proving the theorem.
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</p>
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</details>
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<details id="orgff2611b">
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<summary id="org89a3b1b">
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<details id="org02ee258">
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<summary id="orgf24411c">
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<strong>Formal proof</strong>
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</summary>
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@@ -1851,7 +1851,7 @@ f_{S_R} ({\bf r}) \equiv \frac{1}{4\pi R^2}\oint_{S_R} da' ~ f ({\bf r} + {\bf r
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<p>
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For convenience we will hereafter put \({\bf r} = 0\).
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In spherical coordinates, we have \(da' = R^2 sin \theta d\theta d\phi \equiv R^2 d\Omega\).
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In spherical coordinates, we have \(da' = R^2 sin \theta d\theta d\varphi \equiv R^2 d\Omega\).
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Differentiating with respect to \(R\),
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</p>
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@@ -1931,7 +1931,7 @@ are necessarily positive, we thus require \(f_x > 0\), \(f_y > 0\) and \(f
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of the \(f_x + f_y + f_z = 0\) condition above.
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</p>
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<div class="info div" id="org950ce9d">
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<div class="info div" id="orgfec03b0">
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<p>
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<b>Earnshaw's theorem (physical version)</b> <br>
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It is impossible to find a static distribution of charges which generates an electrostatic field
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@@ -2048,7 +2048,7 @@ 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: 2022-02-13 Sun 21:20</p>
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<p class="date">Created: 2022-02-14 Mon 20:35</p>
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<p class="validation"></p>
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</div>
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