Update 2022-02-14 20:42
This commit is contained in:
+17
-5
@@ -1,7 +1,7 @@
|
||||
<!DOCTYPE html>
|
||||
<html lang="en">
|
||||
<head>
|
||||
<!-- 2022-02-13 Sun 21:20 -->
|
||||
<!-- 2022-02-14 Mon 20:35 -->
|
||||
<meta charset="utf-8">
|
||||
<meta name="viewport" content="width=device-width, initial-scale=1">
|
||||
<title>Pre-Quantum Electrodynamics</title>
|
||||
@@ -1598,14 +1598,26 @@ Table of contents
|
||||
</svg></a><span class="headline-id">ems.ca.sv</span></h4>
|
||||
|
||||
<div class="outline-text-4" id="text-ems_ca_sv">
|
||||
<ul class="org-ul altsecnrs">
|
||||
<li>Gr 3.3</li>
|
||||
</ul>
|
||||
|
||||
|
||||
<p>
|
||||
In many cases, we can't just guess the form of the potential. However, we can often use
|
||||
some symmetry of the problem to greatly simplify the form of solution to Laplace's equation.
|
||||
In many cases, we can't just guess the form of the potential,
|
||||
and calculating it by explicit integration might feel daunting.
|
||||
However, if the setup contains some boundaries which are
|
||||
specified by simple conditions (in the appropriate coordinate
|
||||
system), then the solutions to Laplace's equation factorize
|
||||
into independent (simpler) pieces.
|
||||
</p>
|
||||
|
||||
<p>
|
||||
We illustrate the idea by simple examples.
|
||||
</p>
|
||||
</div>
|
||||
|
||||
|
||||
|
||||
<h5>In this section:</h5>
|
||||
<ul class="child-links-list">
|
||||
<li><a href="ems_ca_sv_car.html">Cartesian Coordinates</a><span class="headline-id">ems.ca.sv.car</span></li>
|
||||
@@ -1628,7 +1640,7 @@ 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: 2022-02-13 Sun 21:20</p>
|
||||
<p class="date">Created: 2022-02-14 Mon 20:35</p>
|
||||
<p class="validation"></p>
|
||||
</div>
|
||||
|
||||
|
||||
Reference in New Issue
Block a user