Update 2022-02-08 17:21
This commit is contained in:
+11
-7
@@ -1,7 +1,7 @@
|
||||
<!DOCTYPE html>
|
||||
<html lang="en">
|
||||
<head>
|
||||
<!-- 2022-02-08 Tue 06:55 -->
|
||||
<!-- 2022-02-08 Tue 17:21 -->
|
||||
<meta charset="utf-8">
|
||||
<meta name="viewport" content="width=device-width, initial-scale=1">
|
||||
<title>Pre-Quantum Electrodynamics</title>
|
||||
@@ -272,6 +272,10 @@ Table of contents
|
||||
</summary>
|
||||
<ul>
|
||||
<li>
|
||||
<a href="./in_t_l.html#in_t_l">Section and equation labelling</a><span class="headline-id">in.t.l</span>
|
||||
|
||||
</li>
|
||||
<li>
|
||||
<a href="./in_t_c.html#in_t_c">Contextual colors</a><span class="headline-id">in.t.c</span>
|
||||
|
||||
</li>
|
||||
@@ -736,7 +740,7 @@ Table of contents
|
||||
|
||||
</li>
|
||||
<li>
|
||||
<a href="./emsm_esm_d.html#emsm_esm_d">Dielectrics</a><span class="headline-id">emsm.esm.d</span>
|
||||
<a href="./emsm_esm_di.html#emsm_esm_di">Dielectrics</a><span class="headline-id">emsm.esm.di</span>
|
||||
|
||||
</li>
|
||||
<li>
|
||||
@@ -1626,7 +1630,7 @@ V_{\mbox{\tiny quad}} ({\bf r}) = \frac{1}{4\pi \varepsilon_0} \frac{1}{r^3} \in
|
||||
\]
|
||||
and can be rewritten as
|
||||
</p>
|
||||
<div class="main div" id="orgd014e56">
|
||||
<div class="main div" id="org7b16036">
|
||||
<p>
|
||||
\[
|
||||
V_{\mbox{\tiny quad}} ({\bf r}) = \frac{1}{4\pi \varepsilon_0} \frac{1}{2} \sum_{a,b} \frac{r_a r_b}{r^5} Q_{ab}
|
||||
@@ -1637,7 +1641,7 @@ and can be rewritten as
|
||||
<p>
|
||||
in terms of the {\bf quadrupole moment}
|
||||
</p>
|
||||
<div class="main div" id="org6f7878a">
|
||||
<div class="main div" id="orga1ea430">
|
||||
<p>
|
||||
\[
|
||||
Q_{ab} = \int_{\cal V} d\tau_s (3 r_{s,a} r_{s,b} - r_s^2 \delta_{a,b}) \rho ({\bf r}_s).
|
||||
@@ -1655,7 +1659,7 @@ Moreover, it is traceless, \(\sum_a Q_{aa} = 0\). It therefore has \(5\) indepe
|
||||
<p>
|
||||
Our expansion for the potential thus looks like
|
||||
</p>
|
||||
<div class="main div" id="org64a7b16">
|
||||
<div class="main div" id="org1059aa3">
|
||||
<p>
|
||||
\[
|
||||
V({\bf r}) = \frac{1}{4\pi \varepsilon_0} \left( \frac{Q}{r} + \sum_a \frac{r_a}{r^3} p_a + \frac{1}{2} \sum_{a,b} \frac{r_a r_b}{r^5} Q_{ab} + ... \right)
|
||||
@@ -1674,7 +1678,7 @@ the leading nonvanishing multipole moment is independent of the chosen location
|
||||
the origin of the coordinate system (see Jackson Prob. 4.4).
|
||||
</p>
|
||||
|
||||
<div class="info div" id="org9ec7af8">
|
||||
<div class="info div" id="org778fe8a">
|
||||
<p>
|
||||
{\bf A consistent nomenclature for the multipole expansion?}\\\\
|
||||
You all know the terms {\bf monopole}, {\bf dipole} and {\bf quadrupole},
|
||||
@@ -1733,7 +1737,7 @@ more terms than you might ever (hopefully) need:<br>
|
||||
|
||||
<hr><div id="postamble" class="status">
|
||||
<p class="author">Author: Jean-Sébastien Caux</p>
|
||||
<p class="date">Created: 2022-02-08 Tue 06:55</p>
|
||||
<p class="date">Created: 2022-02-08 Tue 17:21</p>
|
||||
<p class="validation"><a href="https://validator.w3.org/check?uri=referer">Validate</a></p>
|
||||
</div>
|
||||
|
||||
|
||||
Reference in New Issue
Block a user