<?xml version="1.0"?>
<feed xmlns="http://www.w3.org/2005/Atom" xml:lang="en">
	<id>https://www.wikiwaves.org/index.php?action=history&amp;feed=atom&amp;title=Template%3ANumerical_calculation_of_Q</id>
	<title>Template:Numerical calculation of Q - Revision history</title>
	<link rel="self" type="application/atom+xml" href="https://www.wikiwaves.org/index.php?action=history&amp;feed=atom&amp;title=Template%3ANumerical_calculation_of_Q"/>
	<link rel="alternate" type="text/html" href="https://www.wikiwaves.org/index.php?title=Template:Numerical_calculation_of_Q&amp;action=history"/>
	<updated>2026-04-17T18:57:17Z</updated>
	<subtitle>Revision history for this page on the wiki</subtitle>
	<generator>MediaWiki 1.43.1</generator>
	<entry>
		<id>https://www.wikiwaves.org/index.php?title=Template:Numerical_calculation_of_Q&amp;diff=10859&amp;oldid=prev</id>
		<title>Meylan: /* Numerical Calculation of \mathbf{Q} */</title>
		<link rel="alternate" type="text/html" href="https://www.wikiwaves.org/index.php?title=Template:Numerical_calculation_of_Q&amp;diff=10859&amp;oldid=prev"/>
		<updated>2010-02-10T21:32:29Z</updated>

		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;Numerical Calculation of \mathbf{Q}&lt;/span&gt;&lt;/p&gt;
&lt;table style=&quot;background-color: #fff; color: #202122;&quot; data-mw=&quot;interface&quot;&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;col class=&quot;diff-marker&quot; /&gt;
				&lt;col class=&quot;diff-content&quot; /&gt;
				&lt;tr class=&quot;diff-title&quot; lang=&quot;en&quot;&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;← Older revision&lt;/td&gt;
				&lt;td colspan=&quot;2&quot; style=&quot;background-color: #fff; color: #202122; text-align: center;&quot;&gt;Revision as of 21:32, 10 February 2010&lt;/td&gt;
				&lt;/tr&gt;&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot; id=&quot;mw-diff-left-l25&quot;&gt;Line 25:&lt;/td&gt;
&lt;td colspan=&quot;2&quot; class=&quot;diff-lineno&quot;&gt;Line 25:&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;_{m}\left( s\right) \mathrm{d}s&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;_{m}\left( s\right) \mathrm{d}s&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;/math&amp;gt;&amp;lt;/center&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot;&gt;&lt;/td&gt;&lt;td style=&quot;background-color: #f8f9fa; color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #eaecf0; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&amp;lt;/math&amp;gt;&amp;lt;/center&amp;gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;tr&gt;&lt;td colspan=&quot;2&quot; class=&quot;diff-side-deleted&quot;&gt;&lt;/td&gt;&lt;td class=&quot;diff-marker&quot; data-marker=&quot;+&quot;&gt;&lt;/td&gt;&lt;td style=&quot;color: #202122; font-size: 88%; border-style: solid; border-width: 1px 1px 1px 4px; border-radius: 0.33em; border-color: #a3d3ff; vertical-align: top; white-space: pre-wrap;&quot;&gt;&lt;div&gt;&lt;ins style=&quot;font-weight: bold; text-decoration: none;&quot;&gt;{{reflection and transmission coefficients BEM}}&lt;/ins&gt;&lt;/div&gt;&lt;/td&gt;&lt;/tr&gt;
&lt;/table&gt;</summary>
		<author><name>Meylan</name></author>
	</entry>
	<entry>
		<id>https://www.wikiwaves.org/index.php?title=Template:Numerical_calculation_of_Q&amp;diff=10851&amp;oldid=prev</id>
		<title>Meylan: Created page with &#039;===Numerical Calculation of &lt;math&gt;\mathbf{Q}&lt;/math&gt; ===  We begin by truncating to a finite number (&lt;math&gt;N&lt;/math&gt;) of evanescent modes, &lt;center&gt;&lt;math&gt; \mathbf{Q}\left[ f \right]…&#039;</title>
		<link rel="alternate" type="text/html" href="https://www.wikiwaves.org/index.php?title=Template:Numerical_calculation_of_Q&amp;diff=10851&amp;oldid=prev"/>
		<updated>2010-02-10T21:30:56Z</updated>

		<summary type="html">&lt;p&gt;Created page with &amp;#039;===Numerical Calculation of &amp;lt;math&amp;gt;\mathbf{Q}&amp;lt;/math&amp;gt; ===  We begin by truncating to a finite number (&amp;lt;math&amp;gt;N&amp;lt;/math&amp;gt;) of evanescent modes, &amp;lt;center&amp;gt;&amp;lt;math&amp;gt; \mathbf{Q}\left[ f \right]…&amp;#039;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;===Numerical Calculation of &amp;lt;math&amp;gt;\mathbf{Q}&amp;lt;/math&amp;gt; ===&lt;br /&gt;
&lt;br /&gt;
We begin by truncating to a finite number (&amp;lt;math&amp;gt;N&amp;lt;/math&amp;gt;) of&lt;br /&gt;
evanescent modes,&lt;br /&gt;
&amp;lt;center&amp;gt;&amp;lt;math&amp;gt;&lt;br /&gt;
\mathbf{Q}\left[ f \right] =-\sum_{m=0}^{N}k_{m}\int_{-h}^{0} &lt;br /&gt;
f\left( s\right) \phi_{m}\left( s\right) \mathrm{d}s&lt;br /&gt;
\frac{\phi _{m} \left( z\right)}{A_m} .&lt;br /&gt;
&amp;lt;/math&amp;gt;&amp;lt;/center&amp;gt;&lt;br /&gt;
We calculate the integral&lt;br /&gt;
with the same panels as we used to approximate the integrals of the Green&lt;br /&gt;
function and its normal derivative . Similarly, we&lt;br /&gt;
assume that &amp;lt;math&amp;gt;f(s) \,&amp;lt;/math&amp;gt; is constant over each panel and integrate &amp;lt;math&amp;gt;\phi&lt;br /&gt;
_{m}\left( s\right) &amp;lt;/math&amp;gt; exactly. This gives us the&lt;br /&gt;
following matrix factorisation of &amp;lt;math&amp;gt;\mathbf{Q}&amp;lt;/math&amp;gt; &lt;br /&gt;
&amp;lt;center&amp;gt;&amp;lt;math&amp;gt;&lt;br /&gt;
\mathbf{Q}[f]=\mathbf{S}\,\mathbf{R}\,[f].&lt;br /&gt;
&amp;lt;/math&amp;gt;&amp;lt;/center&amp;gt;&lt;br /&gt;
The components of the matrices &amp;lt;math&amp;gt;\mathbf{S}&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;\mathbf{R}&amp;lt;/math&amp;gt; are &lt;br /&gt;
&amp;lt;center&amp;gt;&amp;lt;math&amp;gt;&lt;br /&gt;
s_{jm} = -k_m\phi _{m}\left( z_{j}\right) ,&lt;br /&gt;
&amp;lt;/math&amp;gt;&amp;lt;/center&amp;gt;&lt;br /&gt;
&amp;lt;center&amp;gt;&amp;lt;math&amp;gt;&lt;br /&gt;
r_{mj} = \frac{1}{A_m} \int_{z_{j}-\Delta x/2}^{z_{j}+\Delta x/2}\phi&lt;br /&gt;
_{m}\left( s\right) \mathrm{d}s&lt;br /&gt;
&amp;lt;/math&amp;gt;&amp;lt;/center&amp;gt;&lt;/div&gt;</summary>
		<author><name>Meylan</name></author>
	</entry>
</feed>