1 Sampling theory

If a continuous-time signal f ( t ) is sampled at terms t = 0 , T , 2 T , n T , then a sequence of values

{ f ( 0 ) , f ( T ) , f ( 2 T ) , f ( n T ) , }

is obtained. The quantity T is called the sample interval or sample period .

Figure 18

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In the previous Sections of this Workbook we have used the simpler notation { f n } to denote a sequence. If the sequence has actually arisen by sampling then f n is just a convenient notation for the sample value f ( n T ) .

Most of our previous results for z-transforms of sequences hold with only minor changes for sampled signals.

So consider a continuous signal f ( t ) ; its z-transform is the z-transform of the sequence of sample values i.e.

{ f ( t ) } = { f ( n T ) } = n = 0 f ( n T ) z n

We shall briefly obtain z-transforms of common sampled signals utilizing results obtained earlier. You may assume that all signals are sampled at 0 , T , 2 T , n T ,

Unit step function

u ( t ) = 1 t 0 0 t < 0

Since the sampled values here are a sequence of 1’s,

{ u ( t ) } = { u n } = 1 1 z 1 = z z 1 z > 1

where { u n } = { 1 , 1 , 1 , } is the unit step sequence.

Ramp function

r ( t ) = t t 0 0 t < 0

The sample values here are

{ r ( n T ) } = { 0 , T , 2 T , }

The ramp sequence   { r n } = { 0 , 1 , 2 , }  has z-transform z ( z 1 ) 2 .

Hence { r ( n T ) } = T z ( z 1 ) 2  since { r ( n T ) } = T { r n } .

Task!

Obtain the z-transform of the exponential signal

f ( t ) = e α t t 0 0 t < 0 .

[Hint: use the z-transform of the geometric sequence { a n } .]

The sample values of the exponential are

{ 1 , e α T , e α 2 T , , e α n T , }

i.e. f ( n T ) = e α n T = ( e α T ) n .

But { a n } = z z a

{ ( e α T ) n } = z z e α T = 1 1 e α T z 1

1.1 Sampled sinusoids

Earlier in this Workbook we obtained the z-transform of the sequence { cos ω n } i.e.

{ cos ω n } = z 2 z cos ω z 2 2 z cos ω + 1

Hence, since sampling the continuous sinusoid

f ( t ) = cos ω t

yields the sequence { cos n ω T } we have, simply replacing ω by ω T in the z-transform:

{ cos ω t } = { cos n ω T } = z 2 z cos ω T z 2 2 z cos ω T + 1
Task!

Obtain the z-transform of the sampled version of the sine wave f ( t ) = sin ω t .

   { sin ω n } = z sin ω z 2 2 z cos ω + 1

{ sin ω t } = { sin n ω T } = z sin ω T z 2 2 z cos ω T + 1

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 T . For example a simple right shift, or delay, of a sampled signal by one sample period is shown in the following figure:

Figure 19

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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 y ( t ) has z-transform Y ( z ) which, as we have seen, really means that its sample values { y ( n T ) } give Y ( z ) , then for y ( t ) shifted to the right by one sample interval the z -transform becomes

{ y ( t T ) } = y ( T ) + z 1 Y ( z )

The proof is very similar to that used for sequences earlier which gave the result:

{ y n 1 } = y 1 + z 1 Y ( z )

Task!

Using the result

{ y n 2 } = y 2 + y 1 z 1 + z 2 Y ( z )

write down the result for { y ( t 2 T ) }

{ y ( t 2 T ) } = y ( 2 T ) + y ( T ) z 1 + z 2 Y ( z )

These results can of course be generalised to obtain { y ( t m T ) } where m is any positive integer.

In particular, for causal or one-sided signals y ( t ) (i.e. signals which are zero for t < 0 ):

{ y ( t m T ) } = z m Y ( z )

Note carefully here that the power of z is still z m not z m T . Examples:

For the unit step function we saw that:

{ u ( t ) } = z z 1 = 1 1 z 1

Hence from the shift properties above we have immediately, since u ( t ) is certainly causal,

{ u ( t T ) } = z z 1 z 1 = z 1 1 z 1 { u ( t 3 T ) } = z z 3 z 1 = z 3 1 z 1

and so on.

Figure 20

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