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	<id>https://fweb.wallawalla.edu/class-wiki/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Andeda</id>
	<title>Class Wiki - User contributions [en]</title>
	<link rel="self" type="application/atom+xml" href="https://fweb.wallawalla.edu/class-wiki/api.php?action=feedcontributions&amp;feedformat=atom&amp;user=Andeda"/>
	<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php/Special:Contributions/Andeda"/>
	<updated>2026-04-05T16:19:09Z</updated>
	<subtitle>User contributions</subtitle>
	<generator>MediaWiki 1.43.0</generator>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=3781</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=3781"/>
		<updated>2004-12-10T23:59:21Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my page describing how a CD Player works.&lt;br /&gt;
&lt;br /&gt;
[[DavidsCD]]&lt;br /&gt;
&lt;br /&gt;
The following links go to things I&#039;ve worked on to get hours for HW#13.  I accumulated 3 hours total.&lt;br /&gt;
&lt;br /&gt;
[[FIR_Filters]]&lt;br /&gt;
&lt;br /&gt;
[[Aliasing]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=3820</id>
		<title>Aliasing</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=3820"/>
		<updated>2004-12-10T23:58:33Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Alaising is what occurs when you sample the highest frequency component of a signal less than two times and then are not able to reconstruct the original signal from the sampled data.  This is generalized by Nyquists sampling theorem that says the signal must be sampled at a frequency of 1/T &amp;gt; 2*fmax.  In the example shown below a wave has a sample period of T and thus a sampling frequency of 1/T.  fmax in this case is greater than 1/2T so there is some overlap in the bandwidth.  This overlap of X(f) will add constructively in the sampled signal.  Now when we wish to convert this sampled signal back to the the original we can not because we have no idea what it orginally looked like, or what frequency components it had.&lt;br /&gt;
&lt;br /&gt;
[[Image:alias.gif]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=269</id>
		<title>Aliasing</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=269"/>
		<updated>2004-12-10T23:56:46Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Alaising is what occurs when you sample the highest frequency component of a signal less than two times and then are not able to reconstruct the original signal from the sampled data.  This is generalized by Nyquists sampling theorem that says the signal must be sampled at a frequency of 1/T &amp;gt; 2*fmax.  In the example shown below a wave has a sample period of T and thus a sampling frequency of 1/T.  fmax in this case is greater than 1/2T so there is some overlap in the bandwidth.  This overlap of X(f) will add constructively in the sampled signal.  Now when we wish to convert this sampled signal back to the the original we can not because we have no idea what it orginally looked like.&lt;br /&gt;
&lt;br /&gt;
[[Image:alias.gif]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=268</id>
		<title>Aliasing</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=268"/>
		<updated>2004-12-10T23:55:43Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Alaising is what occurs when you sample the highest frequency component of a signal less than two times and then are not able to reconstruct the original signal from the sampled data.  This is generalized by Nyquists sampling theorem that says the signal must be sampled at a frequency of 1/T &amp;gt; 2*fmax.  In the example shown below a wave has a sample period of T and thus a sampling frequency of 1/T.  fmax in this case is greater than 1/2T so there is some overlap in the bandwidth.  This overlap of X(f) will add constructively in the sampled.  Now when we wish to convert this sampled signal back to the the original we can not because we have no idea what it orginally looked like.&lt;br /&gt;
&lt;br /&gt;
[[Image:alias.gif]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=267</id>
		<title>Aliasing</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=267"/>
		<updated>2004-12-10T23:46:08Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Alaising is what occurs when you sample the highest frequency component of a signal less than two times and then are not able to reconstruct the original signal from the sampled data.  This is generalized by Nyquists sampling theorem that says the signal must be sampled at a frequency of 1/T &amp;gt; 2*fmax.&lt;br /&gt;
&lt;br /&gt;
[[Image:alias.gif]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Alias.gif&amp;diff=3821</id>
		<title>File:Alias.gif</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Alias.gif&amp;diff=3821"/>
		<updated>2004-12-10T23:45:47Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=261</id>
		<title>Aliasing</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=261"/>
		<updated>2004-12-10T23:22:05Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Alaising is what occurs when you sample the highest frequency component of a signal less than two times and then are not able to reconstruct the original signal from the sampled data.  This is generalized by Nyquists sampling theorem that says the signal must be sampled at a frequency of 1/T &amp;gt; 2*fmax.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=247</id>
		<title>Aliasing</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=Aliasing&amp;diff=247"/>
		<updated>2004-12-10T22:56:38Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;Alaising is what occurs when you are sampling to slow in the time domain.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=270</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=270"/>
		<updated>2004-12-10T22:49:29Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Welcome to David&amp;#039;s Wiki Page! */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my page describing how a CD Player works.&lt;br /&gt;
&lt;br /&gt;
[[DavidsCD]]&lt;br /&gt;
&lt;br /&gt;
The following links go to things I&#039;ve worked on to get hours for HW#13.&lt;br /&gt;
&lt;br /&gt;
[[FIR_Filters]]&lt;br /&gt;
&lt;br /&gt;
[[Aliasing]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=244</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=244"/>
		<updated>2004-12-10T22:48:44Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Welcome to David&amp;#039;s Wiki Page! */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my page describing how a CD Player works.&lt;br /&gt;
&lt;br /&gt;
[[DavidsCD]]&lt;br /&gt;
&lt;br /&gt;
The following link goes to the FIR section I worked on&lt;br /&gt;
&lt;br /&gt;
[[FIR_Filters]]&lt;br /&gt;
&lt;br /&gt;
[[Aliasing]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=3813</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=3813"/>
		<updated>2004-12-10T22:37:04Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Finite Impulse Response Filters */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;br /&gt;
&lt;br /&gt;
Above is shown the Tap Delay Line version of an FIR filter.  It can actually be created in an analog circuit using transmission lines for the T Delay, resistors, an opamp, and an inverting summer to sum them all together.  In the digital sense whats really happening here is that the output of the FIR filter (y(l)) is the convolution of h(l) with x(l) as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:firgarbage.jpg]]&lt;br /&gt;
&lt;br /&gt;
This filter can simply be viewed as a weighted average of the value around the time you are currently at, where h(l) would be the weighting coefficients.  Mathematically it can be viewed as a multiply and accumulate because we are simply taking a predefined impulse function h() and multiplying it by x() then taking the next value of h() and multiplying it by the next value of x().  Then you just sum all those value together and that is the value of some y() at a certain time.  Then you would move forward a step in time and throw out your oldest x() value and bring in the newest x() value to the top of your stack as shown in the picture.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=242</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=242"/>
		<updated>2004-12-10T12:33:01Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;br /&gt;
&lt;br /&gt;
Above is shown the Tap Delay Line version of an FIR filter.  It can actually be created in an analog circuit using transmission lines for the T Delay, resistors, an opamp, and an inverting summer to sum them all together.  In the digital sense whats really happening here is that the output of the FIR filter (y(l)) is the convolution of h(l) with x(l) as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:firgarbage.jpg]]&lt;br /&gt;
&lt;br /&gt;
This filter can simply be viewed as a weighted average of the value around the time you are currently at, where h(l) would be the weighting coefficients.  Mathmatically it can be viewed as a multiply and accumulate becuase we are simply taking a predifined impulse function h() and multiplying it by x() then taking the next value of h() and multiplying it by the next value of x().  Then you just sum all those value together and that is the value of some y() at a certain time.  Then you would move forward a step in time and throw out your oldest x() value and bring in the newest x() value to the top of your stack as shown in the picture.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=213</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=213"/>
		<updated>2004-12-10T12:29:39Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;br /&gt;
&lt;br /&gt;
Above is shown the Tap Delay Line version of an FIR filter.  It can actually be created in an analog circuit using transmission lines for the T Delay, resistors, an opamp, and an inverting summer to sum them all together.  In the digital sense whats really happening here is that the output of the FIR filter (y(l)) is the convolution of h(l) with x(l) as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:firgarbage.jpg]]&lt;br /&gt;
&lt;br /&gt;
This filter can simply be viewed as a weighted average of the value around the time you are currently at, where h(l) would be the weighting coefficients.  Mathmatically it can be viewed as a multiply and accumulate becuase we are simply taking a predifined impulse function h() and multiplying it by x() then taking the next value of h() and multiplying it by the next value of x().  Then you just sum all those value together and that is the value of some y() at a certain time.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=212</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=212"/>
		<updated>2004-12-10T12:22:19Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Finite Impulse Response Filters */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;br /&gt;
&lt;br /&gt;
Above is shown the Tap Delay Line version of an FIR filter.  It can actually be created in an analog circuit using transmission lines for the T Delay, resistors, an opamp, and an inverting summer to sum them all together.  In the digital sense whats really happening here is that the output of the FIR filter (y(l)) is the convolution of h(l) with x(l) as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:firgarbage.jpg]]&lt;br /&gt;
&lt;br /&gt;
It can simply be viewed as a multiply and accumulate becuase we are simply taking a predifined impulse function h(l) which will filter the signal how you want and multiplying it by x(l).&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=211</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=211"/>
		<updated>2004-12-10T12:14:20Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;br /&gt;
&lt;br /&gt;
Above is shown the Tap Delay Line version of an FIR filter.  It can actually be created in an analog circuit using transmission lines for the T Delay, resistors, an opamp, and an inverting summer to sum them all together.  In the digital sense whats really happening here is that the output of the FIR filter (y(l)) is the convolution of h(l) with x(l) as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:firgarbage.jpg]]&lt;br /&gt;
&lt;br /&gt;
It can simply be viewed as a multiply and accumulate becuase we are simply&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Firgarbage.jpg&amp;diff=3815</id>
		<title>File:Firgarbage.jpg</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Firgarbage.jpg&amp;diff=3815"/>
		<updated>2004-12-10T11:53:54Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=210</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=210"/>
		<updated>2004-12-10T11:53:39Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;br /&gt;
&lt;br /&gt;
The output of an FIR filter (y(l)) is the convolution of h(l) with x(l).  It can simply be viewed as a multiply and accumulate.&lt;br /&gt;
&lt;br /&gt;
[[Image:firgarbage.jpg]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=209</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=209"/>
		<updated>2004-12-10T11:47:15Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;br /&gt;
&lt;br /&gt;
The output of an FIR filter (y(l)) is the convolution of h(l) with x(l).  It can simply be viewed as a multiply and accumulate.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=208</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=208"/>
		<updated>2004-12-10T11:28:52Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Finite Impulse Response Filters */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;br /&gt;
[[Image:firtap.jpg]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Firtap.jpg&amp;diff=3814</id>
		<title>File:Firtap.jpg</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Firtap.jpg&amp;diff=3814"/>
		<updated>2004-12-10T11:28:12Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=207</id>
		<title>FIR Filters</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=FIR_Filters&amp;diff=207"/>
		<updated>2004-12-10T11:06:49Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== Finite Impulse Response Filters ==&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=243</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=243"/>
		<updated>2004-12-10T11:06:15Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Welcome to David&amp;#039;s Wiki Page! */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my page describing how a CD Player works.&lt;br /&gt;
&lt;br /&gt;
[[DavidsCD]]&lt;br /&gt;
&lt;br /&gt;
The following link goes to the FIR section I worked on&lt;br /&gt;
&lt;br /&gt;
[[FIR_Filters]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=206</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=206"/>
		<updated>2004-12-10T11:04:35Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Welcome to David&amp;#039;s Wiki Page! */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my page describing how a CD Player works.&lt;br /&gt;
&lt;br /&gt;
[[DavidsCD]]&lt;br /&gt;
&lt;br /&gt;
The following link goes to the FIR section I worked on&lt;br /&gt;
&lt;br /&gt;
[[FIR]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=Signals_and_Systems&amp;diff=221</id>
		<title>Signals and Systems</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=Signals_and_Systems&amp;diff=221"/>
		<updated>2004-12-10T11:00:28Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Topics */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[http://www.wwc.edu/~frohro/ClassNotes/engr455index.htm Class notes for Signals &amp;amp; Systems]&lt;br /&gt;
&lt;br /&gt;
== Topics ==&lt;br /&gt;
*[[Orthogonal functions]]&lt;br /&gt;
*[[Fourier series]]&lt;br /&gt;
*[[Fourier transform]]&lt;br /&gt;
*[[Sampling]]&lt;br /&gt;
*[[Discrete Fourier transform]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
I couldn&#039;t figure out how to get to others Users pages easily so I decided to start posting them here, please add yours:&lt;br /&gt;
&lt;br /&gt;
[[User:Frohro|Rob Frohne]]&lt;br /&gt;
&lt;br /&gt;
[[User:Barnsa|Sam Barnes]]&lt;br /&gt;
&lt;br /&gt;
[[User:Santsh|Shawn Santana]]&lt;br /&gt;
&lt;br /&gt;
[[User:Goeari|Aric Goe]]&lt;br /&gt;
&lt;br /&gt;
[[User:Caswto|Todd Caswell]]&lt;br /&gt;
&lt;br /&gt;
[[User:Andeda|David Anderson]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Davespk.gif&amp;diff=3812</id>
		<title>File:Davespk.gif</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Davespk.gif&amp;diff=3812"/>
		<updated>2004-12-10T10:56:23Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=1424</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=1424"/>
		<updated>2004-12-10T10:53:58Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== CD Players Explained! ==&lt;br /&gt;
&lt;br /&gt;
[[Image:davemic.gif]]&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
[[Image:davespk.gif]]&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Two Times Oversampling ==&lt;br /&gt;
&lt;br /&gt;
Oversampling is the process of interpolating data so that it looks like we have more data than we really do.  Two times oversampling is accomplished by adding a digital interpolation filter right before the DAC.  Now &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt; is convolved with the desired impulse response.  For two times oversampling it would be convolved with &amp;lt;math&amp;gt; h(lt/2) = \frac{T}{2} \int_{-\frac{-1}{T}}^{\frac{1}{T}} e^{(j 2 \pi l t f)/2} df &amp;lt;/math&amp;gt; if we wanted to predistort the signal as well.  This makes it so that the resulting wave in the frequency domain more closely matches the original signal.  So we get more data points doing it this way, we get to filter the signal however we want, plus this allows for the use of a cheaper low pass filter since the frequency spacing is now 2/T.  We just have to be sure and meet the Nyquist criteria now and sample the DAC at T/2 or 88kHz.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Davemic.gif&amp;diff=3811</id>
		<title>File:Davemic.gif</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=File:Davemic.gif&amp;diff=3811"/>
		<updated>2004-12-10T10:53:13Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=203</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=203"/>
		<updated>2004-12-10T10:41:11Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Two Times Oversampling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== CD Players Explained! ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Two Times Oversampling ==&lt;br /&gt;
&lt;br /&gt;
Oversampling is the process of interpolating data so that it looks like we have more data than we really do.  Two times oversampling is accomplished by adding a digital interpolation filter right before the DAC.  Now &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt; is convolved with the desired impulse response.  For two times oversampling it would be convolved with &amp;lt;math&amp;gt; h(lt/2) = \frac{T}{2} \int_{-\frac{-1}{T}}^{\frac{1}{T}} e^{(j 2 \pi l t f)/2} df &amp;lt;/math&amp;gt; if we wanted to predistort the signal as well.  This makes it so that the resulting wave in the frequency domain more closely matches the original signal.  So we get more data points doing it this way, we get to filter the signal however we want, plus this allows for the use of a cheaper low pass filter since the frequency spacing is now 2/T.  We just have to be sure and meet the Nyquist criteria now and sample the DAC at T/2 or 88kHz.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=202</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=202"/>
		<updated>2004-12-10T10:37:26Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* CD Players Explained! */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;== CD Players Explained! ==&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Two Times Oversampling ==&lt;br /&gt;
&lt;br /&gt;
Oversampling is the process of interpolating data so that it looks like we have more data than we really do.  Two times oversampling is accomplished by adding a digital interpolation filter right before the DAC.  Now &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt; is convolved with the desired impulse response.  For two times oversampling it would be convolved with &amp;lt;math&amp;gt; h(lt/2) = \frac{T}{2} \int_{-\frac{-1}{T}}^{\frac{1}{T}} e^{(j 2 \pi l t f)/2} df &amp;lt;/math&amp;gt; if we wanted to predistort the signal as well.  This makes it so that the resulting wave in the frequency domain more closely matches the original signal.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=201</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=201"/>
		<updated>2004-12-10T10:37:13Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Two Times Oversampling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= CD Players Explained! =&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
== Two Times Oversampling ==&lt;br /&gt;
&lt;br /&gt;
Oversampling is the process of interpolating data so that it looks like we have more data than we really do.  Two times oversampling is accomplished by adding a digital interpolation filter right before the DAC.  Now &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt; is convolved with the desired impulse response.  For two times oversampling it would be convolved with &amp;lt;math&amp;gt; h(lt/2) = \frac{T}{2} \int_{-\frac{-1}{T}}^{\frac{1}{T}} e^{(j 2 \pi l t f)/2} df &amp;lt;/math&amp;gt; if we wanted to predistort the signal as well.  This makes it so that the resulting wave in the frequency domain more closely matches the original signal.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=200</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=200"/>
		<updated>2004-12-10T10:32:59Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Two Times Oversampling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= CD Players Explained! =&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
= Two Times Oversampling =&lt;br /&gt;
&lt;br /&gt;
Oversampling is the process of interpolating data so that it looks like we have more data than we really do.  Two times oversampling is accomplished by adding a digital interpolation filter right before the DAC.  Now &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt; is convolved with the desired impulse response.  For two times oversampling it would be convolved with &amp;lt;math&amp;gt; h(lt/2) = \frac{T}{2} \int_{-\frac{-1}{T}}^{\frac{1}{T}} e^{(j 2 \pi l t f)/2} df &amp;lt;/math&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=199</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=199"/>
		<updated>2004-12-10T10:24:44Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Two Times Oversampling */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= CD Players Explained! =&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
= Two Times Oversampling =&lt;br /&gt;
&lt;br /&gt;
Oversampling is the process of interpolating data so that it looks like we have more data than we really do.  Two times oversampling is accomplished by adding a digital interpolation filter right before the DAC.  Now &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt; is convolved with h(t) the desired impulse response.  For two times oversampling h(t) would be by &amp;lt;math&amp;gt;h(lt/2) = frac{T}{2}\int_{-\frac{-1}{T}}^{\frac{1}{T}} e^{j*2*pi*l*t*f\2} \, df &amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=198</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=198"/>
		<updated>2004-12-10T10:17:44Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= CD Players Explained! =&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
= Two Times Oversampling =&lt;br /&gt;
&lt;br /&gt;
Oversampling is the process of interpolating data so that it looks like we have more data than we really do.  Two times oversampling is accomplished by adding a digital interpolation filter right before the DAC.  Now &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt; is convolved with h(t) the desired impulse response.  For two times oversampling it would be &amp;lt;math&amp;gt; h(lt/2) = \frac{T}{2} /int &amp;lt;/math&amp;gt;&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=197</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=197"/>
		<updated>2004-12-10T10:04:29Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;= CD Players Explained! =&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
= Oversampling =&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=196</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=196"/>
		<updated>2004-12-10T09:45:55Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  It has to many high frequency components and would require a really good brick wall filter to get rid of them.  From there the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=195</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=195"/>
		<updated>2004-12-10T09:40:31Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).  From thier the signal is sent to a Low Pass Filter where the stair stepped shaped function is smoothed so that it sounds better when the signal is next sent to the speaker.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=194</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=194"/>
		<updated>2004-12-10T09:34:49Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt; \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=193</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=193"/>
		<updated>2004-12-10T09:32:36Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC) it is convolved with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt; as shown below.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
In the frequency domain you can see that this relates to multipliing &amp;lt;math&amp;gt;\tilde \frac{1}{T} \sum_{n=-\infty}^\infty X(f - \frac{n}{T}) \cdot &amp;lt;/math&amp;gt; by P(f) and results in a quite distored X(f).&lt;br /&gt;
&lt;br /&gt;
&amp;lt;/center&amp;gt;&lt;br /&gt;
where &lt;br /&gt;
&amp;lt;center&amp;gt;&lt;br /&gt;
&amp;lt;math&amp;gt;P(f) = \int_{-\frac{T}{2}}^{\frac{T}{2}} e^{j2\pi ft} \, dt = T sinc(fT)&lt;br /&gt;
&amp;lt;/math&amp;gt;&lt;br /&gt;
&amp;lt;/center&amp;gt;&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; f(t) = \sum_{k= -\infty}^ \infty \alpha_k e^ \frac{j 2 \pi k t}{T} &amp;lt;/math&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=192</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=192"/>
		<updated>2004-12-10T09:26:38Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as &amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  When the data goes through the Digital to Analog Converter (DAC)it is convoluted with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) p (t-KT) &amp;lt;/math&amp;gt;.  &lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; f(t) = \sum_{k= -\infty}^ \infty \alpha_k e^ \frac{j 2 \pi k t}{T} &amp;lt;/math&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=191</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=191"/>
		<updated>2004-12-10T09:24:48Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and is represented mathmatically as ().  When the data goes through the Digital to Analog Converter (DAC)it is convoluted with p(t) to get &amp;lt;math&amp;gt; \tilde x (t) = \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  &lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; f(t) = \sum_{k= -\infty}^ \infty \alpha_k e^ \frac{j 2 \pi k t}{T} &amp;lt;/math&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=190</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=190"/>
		<updated>2004-12-10T08:47:33Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data (x(k*T)) is taken from the CD player and convoluted with p(t) to get&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; \sum_{k= -\infty}^ \infty \ x(kT) \delta (t-KT) &amp;lt;/math&amp;gt;.  &lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&amp;lt;math&amp;gt; f(t) = \sum_{k= -\infty}^ \infty \alpha_k e^ \frac{j 2 \pi k t}{T} &amp;lt;/math&amp;gt;.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=189</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=189"/>
		<updated>2004-12-10T08:38:10Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.&lt;br /&gt;
First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  It does this by basically picking the closest sampling value to the analog value.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
insert pic2&lt;br /&gt;
&lt;br /&gt;
Data is taken from the CD player and represented mathmatically as&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;br /&gt;
(Images by Rob Frohne and resized by Sam Barnes)&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=188</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=188"/>
		<updated>2004-12-10T08:19:25Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.  First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.  Next an analog to digital converter (ADC) samples the data at 44000kHz.  Next this data is stored on a CD.&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
(Images by Rob Frohne and resized by Sam Barnes)&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=187</id>
		<title>DavidsCD</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=DavidsCD&amp;diff=187"/>
		<updated>2004-12-10T08:09:40Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;CD Players Explained!&lt;br /&gt;
&lt;br /&gt;
insert pic1&lt;br /&gt;
&lt;br /&gt;
As seen above storing voice samles on a cd only involves a couple of steps.  First the data must be passed through a low pass filter incase there are any unwanted high frequencies.  In our case we would need a filter to pass anything under 22kHz.  If we pass anything higher than this then there will be alaising.&lt;br /&gt;
&lt;br /&gt;
[[Image:barnsasample.jpg|Sampling a signal]]&lt;br /&gt;
[[Image:barnsaDA.jpg|Digital to analog conversion]]&lt;br /&gt;
(Images by Rob Frohne and resized by Sam Barnes)&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=205</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=205"/>
		<updated>2004-11-18T01:39:46Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Welcome to David&amp;#039;s Wiki Page! */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my page describing how a CD Player works.&lt;br /&gt;
&lt;br /&gt;
[[DavidsCD]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=151</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=151"/>
		<updated>2004-11-18T01:39:14Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my CD Player page.&lt;br /&gt;
&lt;br /&gt;
[[DavidsCD]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=150</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=150"/>
		<updated>2004-11-18T01:38:40Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
&lt;br /&gt;
Click on the link below to go to my CD Player page.&lt;br /&gt;
[[DavidsCD]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=149</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=149"/>
		<updated>2004-09-28T02:11:26Z</updated>

		<summary type="html">&lt;p&gt;Andeda: /* Welcome to David&amp;#039;s Wiki Page! */&lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;br /&gt;
Here there is currently nothing to speak of.&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=100</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=100"/>
		<updated>2004-09-28T02:07:40Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg|thumb|David&#039;s photo]]&lt;br /&gt;
&lt;br /&gt;
== Welcome to David&#039;s Wiki Page! ==&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
	<entry>
		<id>https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=99</id>
		<title>User:Andeda</title>
		<link rel="alternate" type="text/html" href="https://fweb.wallawalla.edu/class-wiki/index.php?title=User:Andeda&amp;diff=99"/>
		<updated>2004-09-28T02:02:23Z</updated>

		<summary type="html">&lt;p&gt;Andeda: &lt;/p&gt;
&lt;hr /&gt;
&lt;div&gt;[[Image:David.jpg]]&lt;/div&gt;</summary>
		<author><name>Andeda</name></author>
	</entry>
</feed>