1 Sampling theory
If a continuous-time signal is sampled at terms then a sequence of values
is obtained. The quantity is called the sample interval or sample period .
Figure 18
In the previous Sections of this Workbook we have used the simpler notation to denote a sequence. If the sequence has actually arisen by sampling then is just a convenient notation for the sample value .
Most of our previous results for z-transforms of sequences hold with only minor changes for sampled signals.
So consider a continuous signal ; its z-transform is the z-transform of the sequence of sample values i.e.
We shall briefly obtain z-transforms of common sampled signals utilizing results obtained earlier. You may assume that all signals are sampled at
Unit step function
Since the sampled values here are a sequence of 1’s,
where is the unit step sequence.
Ramp function
The sample values here are
The ramp sequence has z-transform .
Hence since .
Task!
Obtain the z-transform of the exponential signal
[Hint: use the z-transform of the geometric sequence .]
Earlier in this Workbook we obtained the z-transform of the sequence i.e.
Hence, since sampling the continuous sinusoid
yields the sequence we have, simply replacing by in the z-transform:
Task!
Obtain the z-transform of the sampled version of the sine wave .
1.2 Shift theorems
These are similar to those discussed earlier in this Workbook but for sampled signals the shifts are by integer multiples of the sample period . For example a simple right shift, or delay, of a sampled signal by one sample period is shown in the following figure:
Figure 19
The right shift properties of z-transforms can be written down immediately. (Look back at the shift properties in Section 21.2 subsection 5, if necessary:)
If has z-transform which, as we have seen, really means that its sample values give , then for shifted to the right by one sample interval the -transform becomes
The proof is very similar to that used for sequences earlier which gave the result:
Task!
Using the result
write down the result for
These results can of course be generalised to obtain where is any positive integer.
In particular, for causal or one-sided signals (i.e. signals which are zero for ):
Note carefully here that the power of is still not . Examples:
For the unit step function we saw that:
Hence from the shift properties above we have immediately, since is certainly causal,
and so on.
Figure 20