
- •History
- •Definition
- •Bilateral z-transform
- •Unilateral z-transform
- •Geophysical definition
- •Inverse z-transform
- •Region of convergence
- •Example 1 (no roc)
- •Example 2 (causal roc)
- •Example 3 (anticausal roc)
- •Examples conclusion
- •Properties
- •Initial value theorem
- •Table of common z-transform pairs
- •Relationship to Laplace transform
- •Process of sampling
- •Relationship to Fourier transform
- •Linear constant-coefficient difference equation
- •Transfer function
- •Zeros and poles
- •Output response
- •See also
- •References
Properties
Properties of the z-transform |
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Time domain |
Z-domain |
Proof |
ROC |
Notation |
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ROC:
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Linearity |
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At least the intersection of ROC1 and ROC2 |
Time expansion |
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R^{1/k} |
Time shifting |
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ROC, except
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Scaling in the z-domain |
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Time reversal |
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Complex conjugation |
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ROC |
Real part |
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ROC |
Imaginary part |
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ROC |
Differentiation |
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ROC |
Convolution |
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At least the intersection of ROC1 and ROC2 |
Cross-correlation |
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At least the intersection of ROC of
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First difference |
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At least the intersection of ROC of X1(z)
and
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Accumulation |
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Multiplication |
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Parseval's relation |
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Initial value theorem
,
If
causal
Final value theorem
,
Only if poles of
are
inside the unit circle
Table of common z-transform pairs
Here:
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Signal, |
Z-transform, |
ROC |
1 |
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2 |
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3 |
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4 |
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5 |
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6 |
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7 |
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8 |
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9 |
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10 |
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11 |
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12 |
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13 |
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14 |
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15 |
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16 |
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17 |
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18 |
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19 |
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20 |
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21 |
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Relationship to Laplace transform
The Bilinear transform is a useful approximation for converting continuous time filters (represented in Laplace space) into discrete time filters (represented in z space), and vice versa. To do this, you can use the following substitutions in H(s) or H(z):
from Laplace to z (Tustin transformation), or
from
z to Laplace. Through the bilinear transformation, the complex
s-plane (of the Laplace transform) is mapped to the complex z-plane
(of the z-transform). While this mapping is (necessarily) nonlinear,
it is useful in that it maps the entire
axis
of the s-plane onto the unit
circle in the z-plane. As such,
the Fourier transform (which is the Laplace transform evaluated on
the
axis)
becomes the discrete-time Fourier transform. This assumes that the
Fourier transform exists; i.e., that the
axis
is in the region of convergence of the Laplace transform.