Samping by harrde: Difference between revisions
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==Sampling== |
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Sampling is the process by which an anolog signal is converted into a digital signal and fed into digital circuit. Sampling is done by measuring the analog signal at a regular time interval. Each measurement of the anolog signal is called a sample. We can store and easily manupulate these samples in a computer and then interpolate between the sample points to fully reconstruct the original analog signal when we want to send the signal out of the computer. But we can only reconstruct orignal signal if we have sampled at a rate greater than twice the highest frequency component of the anolog signal. This restriction is given by the Nyquist Theorem which states: |
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===Nyquist Theorem=== |
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A band-limited input signal can be recovered without distortion if it is sampled at a rate of at least twice the highest frequency component of interest within the signal. |
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==How to Sample== |
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For a given input signal x(t) |
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[[Image:InputSignal.jpg]] |
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:we want to sample this at time intervals T. This can be done by multiplying x(t) with a series of impulses |
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[[Image:ImpulseString.jpg]] |
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:given by <math>\sum_{n=-\infty}^{\infty} \delta(t - nT) \ </math>. |
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The product gives us |
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[[Image:ResultSignal.jpg]] |
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which is represented by: <math>\sum_{n=-\infty}^{\infty} x(nT) \delta(t - nT) \ </math> |
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Now we have a digital representation of the signal in a computer as long as the signal is finite in length. The "height" or magnitude of each sample is given by the coeficients x(nT) of each delta funtion. |
Latest revision as of 20:20, 12 November 2007
Sampling
Sampling is the process by which an anolog signal is converted into a digital signal and fed into digital circuit. Sampling is done by measuring the analog signal at a regular time interval. Each measurement of the anolog signal is called a sample. We can store and easily manupulate these samples in a computer and then interpolate between the sample points to fully reconstruct the original analog signal when we want to send the signal out of the computer. But we can only reconstruct orignal signal if we have sampled at a rate greater than twice the highest frequency component of the anolog signal. This restriction is given by the Nyquist Theorem which states:
Nyquist Theorem
A band-limited input signal can be recovered without distortion if it is sampled at a rate of at least twice the highest frequency component of interest within the signal.
How to Sample
- we want to sample this at time intervals T. This can be done by multiplying x(t) with a series of impulses
- given by .
The product gives us which is represented by:
Now we have a digital representation of the signal in a computer as long as the signal is finite in length. The "height" or magnitude of each sample is given by the coeficients x(nT) of each delta funtion.