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j nne e
Chapter 10
The Z-TransformComplex Frequency Domain (Z-Domain) Analysis of LTI System
● Representation of Aperiodic Signals
● Response of LTI System to Aperiodic Signals
j ne §5
特例
推广§10
j nnr e
e
j zz e
r
nz
10.0 Introduction
[ ]y n[ ]x n L
( )jX e
F 1F
( ) ( )j jH e Y e
( )jH e
1
2
3
[ ] ( )jh n H eF
:Key [ ] ( )jx n X eF
2
1[ ] ( )
2
( ) [ ]
j j n
j j n
n
x n X e e d
X e x n e
﹡ Problems: [ ]n
x n
Frequency analysis√
?Frequency analysis
§5
Frequency Domain Analysis
[ ]n
x n
﹡ Condition:
j ne ﹡Cause: Basic signal:
﹡Measure: Basic signal:j nne e
n
nn
represent
√represent
n
( )j ne e ( )j nre nz
z z
Im
Re
②( ) [ ] n
nX z x n z
1[ ] [ ( )]x n Z X z11[ ] ( )
2n
z r
x n X z z dzj
①
10.1 The Z-Transform Pair
A. The Transform Pair [ ] ~ nx n z
[ ] ,n
nx n r
Under Condition we have
( ) [ ( )]X z Z x n
Z a br z r
r
j jz e e re
r e z
( )X z
z-plane
Integral line
j nnr e j nne e
jre
e
Z
ar br
反
正
B. Understanding of The Transform Pairs
11[ ] ( )
2n
z r
x n X z z dzj
2
1[ ] ( )
2j j nnx n X r e r e d
( )( )jj j X reX re e
﹡Inverse Transform
jz re jdz re j d z jd
Frequency
2
1[ ] ( )
2j j nnx n X r e r e d
1 1 2 2[ ] ( ) ( )j j n j j nn nx n X re r e X re r e …… …… ……
11 ( )( )
jj j X reX re e 2
2 ( )( )jj j X reX re e
1cosnr nRe
2cosnr nRe
2nrFrequencynr 1
n n
( ) [ ] n
nX z x n z
﹡The Transform
jz re
( ) [ ] ( )j j nn
nX re x n r e
[ ] n
nx n r
[ ] ~ j nnx n r e ﹡ Similarity :
[ ] ~ j nn nx n r e z ﹡ Similarity :
{ [ ] }nF x n r
Im
Rear
brROC
r
Integralline
[ ] n
nx n r
11[ ] ( )
2n
z r
x n X z z dzj
C. The Convergence Region of the Z-Transform
z
a br r r generally: ROC
点: jre j nnr e :基本信号
2
1[ ] ( )
2j j nnx n X r e r e d
jz re , dz z jd
jz e Let
z 1 if
ROC
11[ ] ( )
2
( ) [ ]
n
z r
n
n
x n X z z dzj
X z x n z
D. Relations Between Z-Transform and Discrete-Time Fourier Transform
2
1[ ] ( )
2
( ) [ ]
j j n
j j n
n
x n X e e d
X e x n e
Z-Transform on Unit Circle
1z
jdz j e d
= Discrete-Time Fourier Transformar
brROC
1r
Im
Rea
ROC
Unit Circle
( )Z zX z
z a
10.2 The Region of Convergence of The Z-Transform
10.2.1 The ROC.
<Examples 10.1>
[ ] [ ]nx n a u n
0 1a ( ) | jz eX z
Z
Condition=ROC
n
[ ]x n
z a
( )jX e
① if ,1a 1z Unit Circle ROC
Im
ReZ a
1a ( ) | jz eX z
② if ,1a
[ ] [ ] ( )n Zz a
zx n a u n X z
z a
( )jX e
一般:右边信号 收敛域向外Z
n
[ ]x n
1z Unit Circle ROC
UnitCircle
1a ( ) | jz eX z
< Examples 10.2> [ ] [ 1]nx n a u n
① if ,1a
Z
Im
Rean
[ ]x n
( )Z zX z
z a
z a
1z Unit Circle ROC
UnitCircle
( )jX e
( ) | jz eX z 1a
② if ,1a
[ ] [ 1] ( )n Zz a
zx n a u n X z
z a
( )jX e
Im
ReZ a
一般:左边信号 收敛域向内Z
n
[ ]x n
1z then the Unit Circle ROC
UnitCircle
<10.1+10.2>
2[ ]x n 1( )X nROC for
Left-sided Right-sided
z a z a1
1
1 az [ ]n Za u n
z
z a<10.1>
[ 1]nZ a u n
<10.2>
( )X Z 2[ ]x n1[ ]x n
1[ ]x nIntegral 2 ( )X nROC for
Im
Rea
Integral
[ ] n
nx n r
Im
Re
Im
Re
10.2.3. General Rule for ROC
, ( ) 'at poles X z doesn t exist
Im
Re
0can be can be
a br z r A. ROC :
B. Poles ROC
z
右边信号
双边信号
左边信号
?
0?
Im
Rear 0r br
0
[ ]x n is two sided
z r
C. ROC 0
a b
a b
r z r
r r r
: ROC
[ ]x n
n
双边信号
环形收敛域或无收敛域
Z
[ ]n
x n b
Im
Re
Unite Circle
b 1/b
<Example 10.7>
0 1b
nbnb
[ ]x n
n
Im
Re
Unite Circle
b1/b
n
[ ]x nnb nb
1b
双边信号 环形收敛域Z 双边信号 无收敛域Z
2
1
1
( )( )Z b z
b z b z b
1
b z b
2
1
( ) [ ]N
n
n NX z x n z
D. is finite duration
z ROC 0z ROC
Im
Re
nz
nz
nz
nz
[ ]x n
n
[ ]x n
n
[ ]x n
n
[ ]x n
Im
Re
Pole at Im
Re
Poles at
0
ROC0z z
“环形” “向内” “向外”
0
ROC: entire Z-plane, 0z
z
possibly except
<Example 10.6 >
,0 1, 0[ ]
0 ,
na n N ax n
else
2
: ( 0 ~ 1)j kNzero ae k N
0 ( 1):
N st orderpole
a
Im
Rea
ROC
0 1N
[ ]x n
n
z a
pole
zero
0
0
Zz z planeexcept z
1
1 N N
n
z a
z az
?
1r
Im
Re0r
E. 0( )r z ROC ( )z ROC?
0nr
1nr
0[ ] n
nx n r
0
[ ]x n is right sided
z r ROC
[ ]x n
n
右边信号 收敛域向外Z
1 0r r
1 0r r1[ ] n
nx n r
Im
Re0r1 0r r
1 0r r
F. 0(0 )z r ROC ( 0 )z ROC
?
1nr
0nr [ ]x n
n
0
[ ]x n is left sided
z r ROC
左边信号 收敛域向内Z
0[ ] n
nx n r
1[ ] n
nx n r
1r
Im
Re
Im
Re
G. Rational
Im
Re
﹡left-sided signal ﹡ Two-sided signal ﹡right-sided signal
( )X z ROC: Bounded by poles
0z ROC ?﹡ z ROC?﹡
10.4 Geometric Evaluation of The Fourier Transform From The Zero-Pole Plot
10.4.1 Geometric Evaluation of Z-Transform
A. The Method
( )( )
( )
B zX z
A z
1
1
0 0
| |( )
| |
( ) ( ) ( )
M
kkN
kk
M N
k kk k
z zX z K
z p
X z z z z p K
零点距离积
极点距离积零点相位和 极点相位和
zero
pole
1
1
( )
( )
M
kkN
kk
z zK
z p
B. Example
1
1( )
1X z
az
Im
Rea
Im
Rea
( )X z
0z
z a
for z a
Im
Re1/2
1
1( )
11
2
X zz
10.4.2 Geometric Evaluation of Fourier Transform
A. The Method
B. Example
( ) | ( )jj
z eX z X e
2 2
( )jX e
( )jX e
if Unit Circle ROC, as above, 1z Let
012
z
z
1
2for z
UnitCircle
jz e
10.5 Properties of Z-Transform
00[ ] ( )nZ
z Rx n n z X z
1 1
2 2
1
2
[ ] ( )
[ ] ( )
Zz R
Zz R
x n X z
x n X z
1 2 1 21 2,[ ] [ ] ( ) ( )Z
z R R R Rax n bx n aX z bX z
[ ] ( )Zz Rx n X z
( 可能加入或去掉)0,z
10.5.1 Linearity k kk k
Za a
10.5.2 Time shifting shift 00
nZn z
11[ ] ( )
2n
z r
x n X z z dzj
[ ] 1Zz z planen
00
11[ ] ( )
2n n
z r
x n n X z z z dzj
<Example>
<Proof>
Z
00[ ] nZ
z z planen n z
Z
[ ] ( )Zz Rx n X z
0
( )z
Xz
0 0( / ) [ ] n n
nX z z x n z z
10.5.3 Scaling in the Z-Domain
( ) [ ] n
nX z x n z
Im
Re0 1z r 0 2z r
Scaling
0z R平移
Im
Re
R
1r 2r
Z
Z
0n Zz
0 1z 外扩
0 1z
or
内收
<Proof>
0 ''
0( )
[ ] Znz RR z R
z x n
[ ] ( )Zz Rx n X z
10.5.4 Time Reversal
'1( ' )
1[ ] ( )Z
z RR
R
x n Xz
( ) [ ] n
nX z x n z
1( ) [ ] n
nX x n z
z
Im
Re
1/R
21/ r 11/ r
Z
Z
Z 1( )z
<Proof>
Im
Re
R
1r 2r
[ ] n
nx n z
[ ] ( )Zz Rx n X z
10.5.5 Time Expansion
( )1/
'( ' )
[ ] ( )k
kk
Zz RR R
x n X z
Where
( )
[ / ][ ]k
x n kx n
, if n is a multiple of k
, else
(时域扩展)Im
Re
1/1
kr 1/2
kr
integer
Z
k=3
-4k -3k -2k -k 0 k 2k 3k 4k补零
( )[ ]kx n
n
[2]x
-4 -3 -2 -1 0 1 2 3 4
[ ]x n
n
[2]x
[ ] ( )Zz R
x n X z
10.5.6 Conjugation
* * *[ ] ( )Zz R
x n X z
For real signal : * *( ) ( )X z X z
Im
Re
Z
[ ] ( )Zz Rx n X z
10.5.7 The Convolution Property
1 1
2 2
1
2
[ ] ( )
[ ] ( )
Zz R
Zz R
x n X z
x n X z
1 2 1 2
1 2
''
[ ] [ ] ( ) ( )Zz RR R R
x n x n X z X z
10.5.8 Differentiation in Z- Domain
[ ] '( )Zz Rnx n zX z ( )
'( )dX z
X zdz
Z
<Example>
1 1
1 2[ ](1 )
n Zz a
n za u n
a az
1
1
1[ ]
1n Z
z aa u naz
1 2
2 1 3
( 1)[ ]
2 (1 )n Z
z an n z
a u na az
Differentiation'( )zX z a
Differentiation , Linear'( )zX z a
Important : useful in Inverse Z-Transform
1[ 1]nZ
z a a u n
1[ 1]nZ
z ana u n
a
1
2
( 1)[ 1]
2nZ
z an n
a u na
<Example>
1( ) log(1 )X z az
1
1
( )
1
dX z azz
dz az
111
1 ( ) [ 1]1
nZz a
aza a u n
az
( )[ ] [ 1]
nax n u n
n
Linearity, Time-scaling
1
1
1( ) [ ]
1nZ
z a a u naz
1[ ] ?Z
z a x n
1[ ]Z
z a nx n
( ) [ 1]na u n
10.5.9 The Initial-value Theorem
10.5.10 Table 10.1 include all properties
10.6 Some Common Z-Transform Pairs
Table 10.2
For causal [ ]x n ( [ ] 0 0)x n for n , we have
( 检验变换的正确性 )
[0] lim ( )z
x X z
,0
lim [ ] n
zn
x n z
1
[ ][0] lim
nzn
x nx
z
10.3 Inverse Z-Transform
1 ( )[ ]
2n
z r
X zx n z dz
j z
① Contour Integral
围线积分Im
Re
ROC
z rIntegral line: ② Partial-Fraction Expansion
部分分式展开
( )X z for any kind of
( )X z for rational
A. Partial-Fraction Expansion for Rational
1. Basic Z-Transform Pairs
( )X z
(10.5.8 example)
1
1
1 az
1
1 2(1 )
z
az
2
1 3(1 )
z
az
1[ ]n Z
z ana u n
a
1[ ]n Z
z aa u n
1
2
( 1)[ ]
2n Z
z an n
a u na
1[ 1]nZ
z a a u n
1[ 1]nZ
z ana u n
a
1
2
( 1)[ 1]
2nZ
z an n
a u na
12 11
1 1 2 1 111 (1 ) (1 ) 1
i i n
i i n
A z AA A
p z p z p z p z
…… ……
2. Idea
( )X z
z①
② Get by Formula in Appendix (Partial-Fraction Expansion)1 ~ nA A
( )X z③
1
1
z
④ [ ]x n
1Z
一阶极点 二阶极点 一阶极点( )
( )
D z
N z 2 11
21 ( )( )
i i n
i ni
A AA A
z p z p z pz p
…… ……
1Z ROC
1 1 2 2 1 1[ ] [ ] [ ] [ ]n ni i i iA x n A x n A x n A x n …… ……
0 1m
ma a z a z ……
2 10 1
mma z a z a z ……
0 1[ 1] [ 2] [ 1]ma n a n a n m ……
B. Examples2 3 8
( )( 2)( 2)( 3)
z zX z
z z z
①( )X z
z
②1 1 1
( )1 2 1 2 1 3
B C DX z A
z z z
1
1
z
1Z
2 / 3 3/ 20 9 / 4 26 /15
1[ ] ?Z x n
2 3 8
( 2)( 2)( 3)
z z
z z z z
2 2 3
A B C D
z z z z
Im
Re-3 2-2BCD
[ ] [ ] [ 2 ( 2) ] [ ] ( 3) [ 1]n n nx n A n B C u n D u n
[ ] [ ] [ 2 ( 2) ( 3) ] [ 1]n n nx n A n B C D u n
[ ] [ ] [ 2 ( 2) ( 3) ] [ ]n n nx n A n B C D u n
③
1Z
for ROC:
for ROC:
Im
Re-3 2-2
Im
Re-2 2-3
for ROC: 2z
2 3z
3 z
左 右
右
BCD
BCD
②1 1 1
( )1 2 1 2 1 3
B C DX z A
z z z
左
10.7 Analysis and Configuration of LTI systems using Z-Transform
10.7.1 System Function of LTI System :
A. Response of LTI System to nz
nz ( ) nH z zLTI
[ ]h n
( )H z
* ,where ( ) [ ] n
nH z h n z
System Function or Transfer Function
System Function
[ ] ( )Zh n H z
( ) ( )n L nH zz H z z
( )H z
B. Explanation of
nz
( )H z
对各衰减因子各频率的衰减复正弦信号的幅度调整和相位调整作用
(类似于 )( )H s
r
je e
ror j nne e 函数集 的选择其中:
( ) ( )n L nH zz H z z
( )H z ( )jH e e
相频特性(给定 )
2 2 2 2
( )jH e e ( )H z
幅频特性(给定 )
j nne e ( )LTIH z [ ( )]( )
jj j n H e enH e e e e ( ) nH z z
<Example>
1
1( )
1H z
az
Im
Rea
Im
Rea
( )H z
Integral Line
jre j nnr e or
j nne e
0z
z a
for z a
r
C. The Method to Obtain
1. From
[ ] ( )Zh n H z ( ) [ ] n
nH z h n z
2. From the Linear-Coefficient Different Equation of LTI System
0 0[ ] [ ]k k
N M
k ka y n k b x n k
, Linearity, Time-Shifting
( )H z
[ ]h n
Z
:
[ ] [ ]Lx n y n
0 0( ) ( )
M
k k
Nk k
k ka z Y z b z X z
[ ] ( )Zx n X z
[ ] ( )kZx n k z X z
0
0
( ) N
Mk
kk
kk
k
b zH z
a z
[ ]* [ ] [ ]x n h n y n
Coefficient of right-side of Equ.
<Example>1 1
[ ] [ 1] [ ] [ 1]2 3
y n y n x n x n
1
1
11
3( )1
12
zH z
z
0 0( ) ( )
M
k k
Nk k
k ka z Y z b z X z
( )( )
( )
Y zH z
X z
Coefficient of left-side of Equ.
[ ]n k kz
( ) ( ) ( )X z H z Y z
10.7.2 System Performance vs.
A. Causality vs.
Causality ROC:
Causality
Rational ROC:
Im
Re
( )H z
( )H z
( )H z
2. including
Cross outermost pole
①
②
Im
Re
① ②
2. Including
1. exterior outside of a circle
1. exterior outside of a circle
B. Stability vs.
Stability 1z
[ ]n
h n
Fourier Transform 1z
( )H z
ROC
ROC( )jH e
jz e
Im
Re
1z Im
Re
1z Im
Re
1z
Stable Unstable Unstable
Im
Re1/2 2
Im
Re1/2 2
Im
Re21/2
1[ ] [( ) 2 ] [ 1]
2n nh n u n
1[ ] ( ) [ ] 2 [ 1]
2n nh n u n u n
1[ ] [( ) 2 ] [ ]
2n nh n u n
Unstable, noncausal Stable, noncausal
Unstable, causal
<Example>
11
1 1( )
1 1 212
H zzz
1z
1z 1z
C. Stable & Causal System ~
Rational
Causality
Stability
z ROCExterior to the circle Acrossing outer most pole
1z ROC
All poles lies inside unit circle 1z
Im
Re1
Unit circle
( )H z
( )H z
10.7.3 Z-Domain Analysis of LTI System
1. Idea
( ) ( )n nLTIH zz H z z
( )[ ] [ ]LTIH zx n y n
: Basic relation between input and output
: Relation between any input and output
1 ( )[ ]
2
1 ( )[ ] ( )
2
n
z r
n
X zx n z dz
j z
X zy n H z z dz
j z
[ ]* [ ] [ ]x n h n y n
( ) ( ) ( )X x H z Y z
① 信号分解 ②已知输入输
出
③ 响应合成
L L
( )Y z
2. Steps
LTI[ ]x n [ ]y n
( )X z ( )Y z( )H z
[ ]h n
( )H zZ 1Z
① ③
②
[ ] ( )Zx n X zKey :
(类似于 域分析)s
① ③
(For zero-state response)
选择合成 的函数集
[ ( )]
2
1( )
2
jj j n Y renY r e r e dj
① :
3. Role of LTI System explained by Z-Domain Analysis
( ) ( ) ( )X z H z Y z( ) ( ) ( )
( ) ( ) ( )
X z H z Y z
X z H z Y z
jz r e
幅度调整
相位调整
[ ( )]
2
1[ ] ( )
2
jj j n X renx n X r e r e dj
[ ]y n
( )H z ( )jH r e
( )jH re
[ ]x nr
( )H z
j nnr e
调整幅度 调整相位L
② :
规定了每个函数集的幅相调整方法
4. Example
[ ] ( 3) [ ]nh n u n , [ ] [ ]x n u n :求 [ ] ?y n
<Solution>
LTI[ ]u n ?
11 z
1
1
1 3z
( 3) [ ]nu n
1
1
1 3z Z 1Z
① ③
②
( 3)z 1z 3z
3 1
[ ( 3) ] [ ]4 4
n u n
1 1(1 3 )(1 )z z
1Z 3z
1 1
(3 / 4) (1/ 4)
1 3 1z z
10.8 System Function Block Program of LTI System
10.9 The Unilateral Laplace Transform
10.9.1 Definition
0| |[ ] ( )uuZ
z rx n X z 0
1
| |
( ) [ ]
1[ ] ( )
2
nu
n
nu
Z r
X z x n z
x n X z z dzj
i.e.
( 0)n
[ ]x n
[ ], 0[ ]
0 ,u
x n nx n
else
uZ
单边化
0| |z rZ
, 0[ ]
?, 0
nx n
n
√
( )uX s ( )uX s
1
uZ
[ ] [ ]x n u n
单边化①
②
<10.32>
[ ] [ ]nx n a u n
[ ] [ ]ux n x nuZ
| | | |z aZ
1
1( )
1uX zaz
causal
For causal signal
Z
uZ ( )uX z
( )X z
[ ]ux n
[ ]x n
<10.33>
For non-causal signal
Z
uZ ( )uX z
( )X z
1[ ] [ 1]nx n a u n
[ ] [ ]nux n a a u n u
Z
单边化
| | | |z aZ
1( )
1u
aX z
az
non-causal
Z
[ ]x n
11
z
az
| | | |z a
1| | | |1
[ ]1
nz aZa u n
az
| | | |z aZ
1| | | | ( )1uz a
Z aX z
az
2
1
uZ
[ ]ux n
[ ]x n
0n
[ ]x n1 [ 1]na u n
n
n
[ ]ux n 1[ ]na a u n
①
②
1( )
1
zX z
az
Im
Re
Im
Re
10.9.2 Properties of Unilateral Z-Transform
Table 10.3 (Compared to Table 10.1) Difference
A. Roc:
( )uX z ( )urational X zB. Time Reversal:
Don’t exist
C. Convolution:
11
22
1
2|
| |
|
[ ] ( )
[ ] ( )
u
u
u
uz
z r
r
x n X z
x n X z
Z
Z
1 2[ ] [ ]if x n and x n are causal
1 21 2
1 2)| | max( ,[ ] [ ] ( ) ( )uu uz r rx n x n X z X zZ
D. Time Shifting:
0| |[ ] ( )uuz r
Zx n X z
0
1| |[ 1] ( ) [ 1]u
uz rZx n z X z x
0| |[ 1] ( ) [0]uuz r
Zx n zX z zx
10.9.3 Solving Difference Equation Using the Unilateral Z-Transform
<10.37> Causal LTI System
11( ) 3 ( ) 3 [ 1]
1u uY z z Y z yz
1 1 1
3( )
1 3 (1 3 )(1 )uY zz z z
uZ inputstate
Zero input response Zero state response
[ ] 3 [ 1] [ ]y n y n x n , 0
[ ]?, 0
nx n
n
[ 1]y , ,
Full Response
Causal
ROC
① If 8, 1
1 1
3 2( )
1 3 1uY zz z
[ ] [3 ( 3) 2] [ ]nuy n u n
[ ] 3 ( 3) 2ny n 0for n
1uZ
② If 0
1 1( )
(1 3 )(1 )uY zz z
3 1
[ ] [ ( 3) ] [ ]4 4
nuy n u n
0for n
1uZ
(zero-state)
3 1[ ] [ ( 3) ]
4 4ny n
Causal
ROC
Im
Re1-3
Im
Re1-3
(Full Response)
1 1
(3/ 4) (1/ 4)
1 3 1z z
* Alternative Way of Solving Zero-State Response: when [ ] [ ]x n u n
1
1( )
1 3H z
z
| | 3z
1( )
1X z
z
| | 1z
1 1( )
(1 3 )(1 )Y z
z z
| | 3z
3 1[ ] [ ( 3) ] [ ]
4 4ny n u n
1Z
Causal →ROC
实际未说明初始状态都是零状态
Im
Re-3 1
Im
Re1
Im
Re-3
[ ]x n for n