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3/28/2014
1
KCEC 2117
Control Engineering
Analyses of Transient and Steady State
Time response
Dr. Yap Hwa Jen
What is next
 After modeling, we look at the response of the system
based on the input
 Some fundamental properties of systems
 1st order
 2nd order
2
3/28/2014
2
Transient and steady-state response
y(t) = ytr (t)
transient
+ yss (t)
steady state
3
Steady-state response
 The final value of the system, should the system is stable
 Can also be found by FinalValue Theorem
 When is the FVT applicable?
 F(s) should have no poles in the right half of the complex plane (Real part should not be +v).
 F(s) should have no poles on the imaginary axis, except at most one pole at s=0.
 E.g.
lim
t®¥
f (t) = lim
s®0
sF(s);
only if lim
t®¥
f (t) is finite
4
no)(
yes)(
2


s
A
sF
s
A
sF
3/28/2014
3
Steady-state response
 Another use of FVT is to calculate DC gain
 DC gain is the ratio of output to input after all transients
have decayed
 Assume input is unit step
)(lim;
1
)(lim=gainDC
00
sF
s
ssF
ss 

5
1st order systems
 Example:
 RC circuit
 Thermal systems
 Assume zic
C(s)
R(s)
=
1
Ts+1
6
3/28/2014
4
1st order systems: unit step response
Tt
etc
sTs
sC
TssR
sC
/
1)(
1
1
1
)(
1
1
)(
)(








7
T
e
Tdt
dc
t
Tt
t
11
:0)(tSlope
0
/
0 




1st order systems: unit ramp response
Tt
TeTttc
sTs
sC
/
2
)()(
1
1
1
)(





8
 
     
 
  Te
eTte
tctrte
te
Tt




and
)1(
thenis,signal,errorThe
/
3/28/2014
5
1st order systems: unit impulse response
C(s) =
1
Ts +1
1
c(t) =
1
T
e-t/T
9
Specifications
 Rise time, tr (10%-90%)
 Settling time, ts (2% or 5%)
 Time constant,T or t
10
3/28/2014
6
Example
11
Characteristics of First Order Systems
Example: Obtain the
transfer function of the
system shown in Figure
(s)/T(s) and find its
time constant and the
final value under unit
step input, J=0.01 Kgm2
and B=0.04
Characteristics of First Order Systems
Solution
1250
25
4
100
040010
1
1
ss
s.
BJssT
s
.
.
)(
)(
The time constant =0.25sec
The final value= 25rad/sec
0 0.5 1 1.5
0
5
10
15
20
25
StepResponse
Time(sec)
Amplitude
11
Example
11
Characteristics of First Order Systems
Example: Obtain the
transfer function of the
system shown in Figure
(s)/T(s) and find its
time constant and the
final value under unit
step input, J=0.01 Kgm2
and B=0.04
Characteristics of First Order Systems
Solution
1250
25
4
100
040010
1
1
ss
s.
BJssT
s
.
.
)(
)(
The time constant =0.25sec
The final value= 25rad/sec
0 0.5 1 1.5
0
5
10
15
20
25
StepResponse
Time(sec)
Amplitude
12
3/28/2014
7
2nd order system
b
u(t)
s
m
k
s
m
b
s
m
skbsms
sX
s
sU
kbsmssU
sX
1
1
11
)(
;
1
)(let
1
)(
)(
2
2
2













13
2nd order system
m =1,b = 2,k = 5
X(s)
U(s)
=
1
s2
+ 2s+ 5
Case 1:
14
3/28/2014
8
2nd order system
m =1,b = 2,k =1
X(s)
U(s)
=
1
s2
+ 2s+1
Case 2:
15
2nd order system
m =1,b = 4,k = 3
X(s)
U(s)
=
1
s2
+ 4s+3
Case 3:
16
3/28/2014
9
2nd order system
n
nn
nn
n
ss
sssR
sC





frequency,natural
ratio,damping
02:equationsticCharacteri
2)(
)(
22
22
2



17
2nd order system
18
 







 














2
1
2
2
1
tanshift,phase
1frequency,naturaldamped
where
sin
1
1
1)(
nd
d
t
tety n
 In general, the output response with a unit step input &
zic:
3/28/2014
10
Various damping ratios
19
2nd order systems
Case ζ Roots of
characteristic
equation
Example
Case 1:
Underdamped
Pair of complex
poles
Case 2:
Critically damped
Two equal poles
Case 3:
Overdamped
Two distinct,
negative real poles
0 <z <1 s = -1± j2
z >1
z =1
s = -1,-2
s = -1,-1
20
3/28/2014
11
2nd order system: characteristics
21
2nd order system: specifications
 Rise time, tr (10%-90%)
 Settling time, ts (2% or 5%)
 Delay time, td (0%-50%)
 Peak time, tp
 Maximum (percent) overshoot, Mp
 These specifications can be determined from the plot of
the response. Additionally these specifications also apply
for systems of higher orders.
22
3/28/2014
12
Transient response specifications
(for 2nd order systems)
 Rise time,
 Peak time,
 Max overshoot,
 Setting time,
2
1, 




 nd
d
rt
d
pt

















2
1
eM p
criterion)(2%
4
n
st


23
Tutorials
24
1. Case-4: m=1, b=0, k=1
2. For all Cases (1, 2, 3 and 4), find the
 time response equation, y(t)
 damping ratio (ζ) and natural frequency (ωn)
 damped natural frequency (ωd)
 Rise time (tr), Peak time (tp) & Setting time (ts)
 Max overshoot (Mp)
3/28/2014
13
Poles and zeros
 Say we have a transfer function of a system:
 The zero(s) of the system are the roots of the numerator
 The pole(s) of the system are the roots of the
denumerator/characteristic eqn.
 What are the zeros of the system above? What are the
poles?
 What is the order of the system?
)3)(2(
1
)(



ss
s
sG
25
Pole zero map
 It is convenient to draw the pole(s) and zero(s) of the
system in a graphical manner
)3)(2(
1
)(



ss
s
sG
26
3/28/2014
14
Example
 Draw the pole-zero map (pzmap) of this system
)52)(5(
)2)(5.0(
)(



sss
ss
sG
27
Example
28
3/28/2014
15
Effects of pole(s) position
 Let’s start with a simple, 1st order system
 What is the pole of the system?
 Plot the pzmap and the response of the system to a unit
step input
1
1
)(1


s
sG
29
30
3/28/2014
16
Effects of pole(s) position
 Another system
2
2
)(2


s
sG
31
Effects of pole(s) position
 What about G3? What is the expected response?
 What is your conclusion from this?
10
10
)(3


s
sG
32
3/28/2014
17
Effects of pole(s) position
 What if we have a pole on the right half plane (RHP) of
the pzmap? Eg.:
1
1
)(4


s
sG
33
What can be concluded from the info about the position
of the pole on the pzmap?
34
3/28/2014
18
Finding:
A system is stable only if all the poles of
the system are located in the LHP of the
pzmap!
35
Effect of pole position
 Do the same to 2nd order systems
 Remember we have 3 cases for 2nd order systems:
underdamped, critically damped and overdamped
36
3/28/2014
19
Effect of pole position
 An example 2nd order system:
 What are the poles of this system? Write the complex
pole in terms of
 Compare the denumerator with the standard
characteristic eqn. for a 2nd order system:
 How are these related to each other? :
)1)(1(
1
22
1
)( 21
jsjsss
sG




djs  
02 22
 nnss 
dn  ,,,
37
Effect of pole position
z = cosb
wn = wd
2
+s 2
wd =wn 1-z2
s =zwn
38
3/28/2014
20
Time function vs pole location
39
Effects of zero locations
 The zero affects the transient response:
 Example: G2 has a zero near a pole:
tt
tt
eetg
ssss
s
sG
eetg
ssss
sG
2
2
2
2
1
1
64.118.0)(
2
64.1
1
18.0
)2)(1(1.1
)1.1(2
)(
22)(
2
2
1
2
)2)(1(
2
)(

















40
3/28/2014
21
Effects of zero locations
G1 G2
41
Effects of zero locations
 Time response plot:
Generally, a zero near
a pole reduces the
amount of that term
in the total response
42
3/28/2014
22
Effect of zero location
 Observe these two systems, one with zero in RHP







)(
)42.11)(42.11(
)1(1
)(
)(
)42.11)(42.11(
1
)(
2
2
1
1
th
jsjs
s
sH
th
jsjs
sH
43
Effect of zero location
 Observe these two systems, one with zero in RHP
A zero in the RHP results
in an initial opposite
response  non-
minimum phase system
44

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time response

  • 1. 3/28/2014 1 KCEC 2117 Control Engineering Analyses of Transient and Steady State Time response Dr. Yap Hwa Jen What is next  After modeling, we look at the response of the system based on the input  Some fundamental properties of systems  1st order  2nd order 2
  • 2. 3/28/2014 2 Transient and steady-state response y(t) = ytr (t) transient + yss (t) steady state 3 Steady-state response  The final value of the system, should the system is stable  Can also be found by FinalValue Theorem  When is the FVT applicable?  F(s) should have no poles in the right half of the complex plane (Real part should not be +v).  F(s) should have no poles on the imaginary axis, except at most one pole at s=0.  E.g. lim t®¥ f (t) = lim s®0 sF(s); only if lim t®¥ f (t) is finite 4 no)( yes)( 2   s A sF s A sF
  • 3. 3/28/2014 3 Steady-state response  Another use of FVT is to calculate DC gain  DC gain is the ratio of output to input after all transients have decayed  Assume input is unit step )(lim; 1 )(lim=gainDC 00 sF s ssF ss   5 1st order systems  Example:  RC circuit  Thermal systems  Assume zic C(s) R(s) = 1 Ts+1 6
  • 4. 3/28/2014 4 1st order systems: unit step response Tt etc sTs sC TssR sC / 1)( 1 1 1 )( 1 1 )( )(         7 T e Tdt dc t Tt t 11 :0)(tSlope 0 / 0      1st order systems: unit ramp response Tt TeTttc sTs sC / 2 )()( 1 1 1 )(      8             Te eTte tctrte te Tt     and )1( thenis,signal,errorThe /
  • 5. 3/28/2014 5 1st order systems: unit impulse response C(s) = 1 Ts +1 1 c(t) = 1 T e-t/T 9 Specifications  Rise time, tr (10%-90%)  Settling time, ts (2% or 5%)  Time constant,T or t 10
  • 6. 3/28/2014 6 Example 11 Characteristics of First Order Systems Example: Obtain the transfer function of the system shown in Figure (s)/T(s) and find its time constant and the final value under unit step input, J=0.01 Kgm2 and B=0.04 Characteristics of First Order Systems Solution 1250 25 4 100 040010 1 1 ss s. BJssT s . . )( )( The time constant =0.25sec The final value= 25rad/sec 0 0.5 1 1.5 0 5 10 15 20 25 StepResponse Time(sec) Amplitude 11 Example 11 Characteristics of First Order Systems Example: Obtain the transfer function of the system shown in Figure (s)/T(s) and find its time constant and the final value under unit step input, J=0.01 Kgm2 and B=0.04 Characteristics of First Order Systems Solution 1250 25 4 100 040010 1 1 ss s. BJssT s . . )( )( The time constant =0.25sec The final value= 25rad/sec 0 0.5 1 1.5 0 5 10 15 20 25 StepResponse Time(sec) Amplitude 12
  • 8. 3/28/2014 8 2nd order system m =1,b = 2,k =1 X(s) U(s) = 1 s2 + 2s+1 Case 2: 15 2nd order system m =1,b = 4,k = 3 X(s) U(s) = 1 s2 + 4s+3 Case 3: 16
  • 9. 3/28/2014 9 2nd order system n nn nn n ss sssR sC      frequency,natural ratio,damping 02:equationsticCharacteri 2)( )( 22 22 2    17 2nd order system 18                          2 1 2 2 1 tanshift,phase 1frequency,naturaldamped where sin 1 1 1)( nd d t tety n  In general, the output response with a unit step input & zic:
  • 10. 3/28/2014 10 Various damping ratios 19 2nd order systems Case ζ Roots of characteristic equation Example Case 1: Underdamped Pair of complex poles Case 2: Critically damped Two equal poles Case 3: Overdamped Two distinct, negative real poles 0 <z <1 s = -1± j2 z >1 z =1 s = -1,-2 s = -1,-1 20
  • 11. 3/28/2014 11 2nd order system: characteristics 21 2nd order system: specifications  Rise time, tr (10%-90%)  Settling time, ts (2% or 5%)  Delay time, td (0%-50%)  Peak time, tp  Maximum (percent) overshoot, Mp  These specifications can be determined from the plot of the response. Additionally these specifications also apply for systems of higher orders. 22
  • 12. 3/28/2014 12 Transient response specifications (for 2nd order systems)  Rise time,  Peak time,  Max overshoot,  Setting time, 2 1,       nd d rt d pt                  2 1 eM p criterion)(2% 4 n st   23 Tutorials 24 1. Case-4: m=1, b=0, k=1 2. For all Cases (1, 2, 3 and 4), find the  time response equation, y(t)  damping ratio (ζ) and natural frequency (ωn)  damped natural frequency (ωd)  Rise time (tr), Peak time (tp) & Setting time (ts)  Max overshoot (Mp)
  • 13. 3/28/2014 13 Poles and zeros  Say we have a transfer function of a system:  The zero(s) of the system are the roots of the numerator  The pole(s) of the system are the roots of the denumerator/characteristic eqn.  What are the zeros of the system above? What are the poles?  What is the order of the system? )3)(2( 1 )(    ss s sG 25 Pole zero map  It is convenient to draw the pole(s) and zero(s) of the system in a graphical manner )3)(2( 1 )(    ss s sG 26
  • 14. 3/28/2014 14 Example  Draw the pole-zero map (pzmap) of this system )52)(5( )2)(5.0( )(    sss ss sG 27 Example 28
  • 15. 3/28/2014 15 Effects of pole(s) position  Let’s start with a simple, 1st order system  What is the pole of the system?  Plot the pzmap and the response of the system to a unit step input 1 1 )(1   s sG 29 30
  • 16. 3/28/2014 16 Effects of pole(s) position  Another system 2 2 )(2   s sG 31 Effects of pole(s) position  What about G3? What is the expected response?  What is your conclusion from this? 10 10 )(3   s sG 32
  • 17. 3/28/2014 17 Effects of pole(s) position  What if we have a pole on the right half plane (RHP) of the pzmap? Eg.: 1 1 )(4   s sG 33 What can be concluded from the info about the position of the pole on the pzmap? 34
  • 18. 3/28/2014 18 Finding: A system is stable only if all the poles of the system are located in the LHP of the pzmap! 35 Effect of pole position  Do the same to 2nd order systems  Remember we have 3 cases for 2nd order systems: underdamped, critically damped and overdamped 36
  • 19. 3/28/2014 19 Effect of pole position  An example 2nd order system:  What are the poles of this system? Write the complex pole in terms of  Compare the denumerator with the standard characteristic eqn. for a 2nd order system:  How are these related to each other? : )1)(1( 1 22 1 )( 21 jsjsss sG     djs   02 22  nnss  dn  ,,, 37 Effect of pole position z = cosb wn = wd 2 +s 2 wd =wn 1-z2 s =zwn 38
  • 20. 3/28/2014 20 Time function vs pole location 39 Effects of zero locations  The zero affects the transient response:  Example: G2 has a zero near a pole: tt tt eetg ssss s sG eetg ssss sG 2 2 2 2 1 1 64.118.0)( 2 64.1 1 18.0 )2)(1(1.1 )1.1(2 )( 22)( 2 2 1 2 )2)(1( 2 )(                  40
  • 21. 3/28/2014 21 Effects of zero locations G1 G2 41 Effects of zero locations  Time response plot: Generally, a zero near a pole reduces the amount of that term in the total response 42
  • 22. 3/28/2014 22 Effect of zero location  Observe these two systems, one with zero in RHP        )( )42.11)(42.11( )1(1 )( )( )42.11)(42.11( 1 )( 2 2 1 1 th jsjs s sH th jsjs sH 43 Effect of zero location  Observe these two systems, one with zero in RHP A zero in the RHP results in an initial opposite response  non- minimum phase system 44