Update 2022-02-15 10:32

2022-02-15 10:32:42 +01:00
parent 09a8ba5fb6
commit 6874e66024
204 changed files with 1019 additions and 937 deletions
@@ -1,7 +1,7 @@
 <!DOCTYPE html>
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 <head>
-<!-- 2022-02-14 Mon 20:35 -->
+<!-- 2022-02-15 Tue 10:14 -->
 <meta charset="utf-8">
 <meta name="viewport" content="width=device-width, initial-scale=1">
 <title>Pre-Quantum Electrodynamics</title>
@@ -1621,7 +1621,7 @@ B^{\parallel}_{above} - B^{\parallel}_{below} = \mu_0 K
 So:  component of \({\bf B}\) that is parallel to surface but perpendicular to current flow
 is discontinuous, whereas the one parallel to the flow is continuous.  In vector notation:
 </p>
-<div class="main div" id="org52ffa1f">
+<div class="main div" id="org7837ca0">
 <p>
 \[
    {\bf B}_{above} - {\bf B}_{below} = \mu_0 {\bf K} \times \hat{\bf n},
@@ -1633,7 +1633,7 @@ is discontinuous, whereas the one parallel to the flow is continuous.  In vector
 <p>
 where \(\hat{\bf n}\) points upwards. For the vector potential, the relations are
 </p>
-<div class="main div" id="orgbc3e08a">
+<div class="main div" id="org4d288c9">
 <p>
 \[
    {\bf A}_{above} = {\bf A}_{below}
@@ -1679,7 +1679,7 @@ What is left is
 \]
 Therefore, reidentifying the normal component, we get
 </p>
-<div class="main div" id="org7cf5c86">
+<div class="main div" id="org2c3962c">
 <p>
 \[
    \frac{\partial {\bf A}_{above}}{\partial n} - \frac{\partial {\bf A}_{below}}{\partial n}
@@ -1709,7 +1709,7 @@ 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: 2022-02-14 Mon 20:35</p>
+<p class="date">Created: 2022-02-15 Tue 10:14</p>
 <p class="validation"></p>
 </div>