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		<title>Pridma at 05:16, 26 October 2007</title>
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		<updated>2007-10-26T05:16:43Z</updated>

		<summary type="html">&lt;p&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;==About Sampling==&lt;br /&gt;
It is impossible to store all possible information about a waveform in a computer. The function on any interval has an infinite amount of points inside that interval. We need a way of storing a waveform inside finite memory. This can be accomplished through the awesomeness of something called sampling. With some restrictions, mentioned below, you can take the magnitude of the waveform at a given time interval, store it, and be able to reproduce the the same waveform through Fourier Transforms.&lt;br /&gt;
&lt;br /&gt;
==Restrictions==&lt;br /&gt;
When you sample, you must first band-limit your input waveform before you sample. Otherwise, you&amp;#039;ll get a lot of artifacts.&lt;br /&gt;
&lt;br /&gt;
===Why you must band-limit the input===&lt;br /&gt;
When you look at the Fourier Transform of an example input waveform, you&amp;#039;ll get a semicircle. After you sample, the semicircle will be periodic. If you do not band-limit the input wavevform, the semicircles may overlap, and if that happens, there is no way of knowing what part of each semicircle is where. You won&amp;#039;t be able to tell the difference between each semicircle.&lt;br /&gt;
&lt;br /&gt;
==Nyquist Theorem==&lt;br /&gt;
If you sample a band-limited signal at a sample rate greater than 2 times the highest frequency component of the input waveform, you won&amp;#039;t lose any information about the signal and you&amp;#039;ll be able to reconstruct the waveform from the samples.&lt;/div&gt;</summary>
		<author><name>Pridma</name></author>
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