Discrete-time Systems in the Time Domain Domain
Chapter 4 Chapter 4 Sections 4.1 - 4.7
- Dr. Iyad Jafar
Discrete-time Systems in the Time Domain Domain Chapter 4 Chapter - - PowerPoint PPT Presentation
Discrete-time Systems in the Time Domain Domain Chapter 4 Chapter 4 Sections 4.1 - 4.7 Dr. Iyad Jafar Outline Outline Definition Examples Classification of Discrete-time Systems Impulse and Step Responses Linear
2
3
4
1.5 x[n] y[n] 0.5 1 [ n ] y[ ]
x[
M=3
5
5 10 15 20
n
6
7
U li
3 4 ] 3 4 ]
Up-sampling
1 2 x[ n ] 1 2 y[ n ] 2 4 6 8 10 12 n 2 4 6 8 10 12 n
Interpolation
3 4 1 2 z[ n ]
8
2 4 6 8 10 12 n
1[ ]
9
10
x[n / L] , n = 0, L, 2L, 3L ... y[n] 0 , otherwise
⎨ ⎩
11
12
13
2 2
n n
2 n n
14
15
16
17
Linear Time-Invariant (LTI) System -A system satisfying
LTI systems are mathematically easy to analyze and
There are highly useful signal processing algorithms have
Linear
18
19
Hence because of the linearity property we get
Now, any arbitrary input sequence x[n] can be expressed as a
20
The response of the LTI system to an input x[k]δ[n − k] will
As we discussed in Chapter 2 this summation is called the As we discussed in Chapter 2, this summation is called the
21
1 2 1 2
22
Stability of LTI Systems
n
S | h[n]|
23
Stability of LTI Systems
24
Causality of LTI Systems
25
Interconnection of LTI Systems
1.
1.
26
Interconnection of LTI Systems
27
Interconnection of LTI Systems
2.
2.
28
Interconnection of LTI Systems
h3[n]
h1[n] h [n] + x[n] y[n]
h2[n]
29
LTI systems may have finite impulse response (FIR) such that
2 1
N k N
y[n] h[k] x[n-k]
1
k N
M 1
1 y[n] x[n-k]
M 1
1 h[n] [n-k]
30
k 0
y[ ] [ ] M
k 0
[ ] [ ] M
On the other hand, some LTI systems have infinite impulse
n
k 0
31
One popular and important class of LTI systems can be
The order of the difference equation is max(M,N)
Such systems are usually IIR systems in general
32
Example 3.12:
33
For a LTI system described by a LCCDE, we can determine
However, can we find y[n] in a closed form
34
The solution of a LCCDE can be expressed as The
The
The particular (non-homogeneous, forced response, steady
35
Computation of yc[n] Assumes x[n] = 0 and yc[n] = λn , thus, the LCCDE becomes The polynomial factors into (λ λ )(λ λ )
The polynomial factors into (λ-λ1)(λ-λ2)… = 0, with each λi
Thus, the complementary solution becomes
36
In case the root has multiplicity of L, the complementary
37
Computation of yp[n] The particular solution assumes the same form of x[n] scaled
x[n] = A u[n] yp[n] = β u[n] x[n] = An u[n] yp[n] = β An u[n] x[n] = A cos(ωon) yp[n] = β cos(ωon)
If the assumed solution for yp[n] is the same as the
x[n] = 3n u[n] and yh[n] = 3n +2n yp[n] = β n 3n u[n]
38
Example 3.15: Solve the following LCCDE
39
Example 3.16: Solve the following LCCDE
40
Example 3.17: Solve the following LCCDE
41
Stability of LTI Systems - Revisited
42
43