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System Responses
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Two parts:
Steady-state Response Transient response
System Responses
u
bK
Mx
Transient response
Steady State Response
Input:
Output:
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First Order System
The first order system has only one pole.
Where K is the D.C gain and T is the time constantof the system.
Time constant is a measure of how quickly a 1storder system responds to a unit step input.
D.C Gain of the system is ratio between the inputsignal and the steady state value of output.
1TsK
sRsC)()(
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Introduction
The first order system given below.
1310
s
sG )(
5
3
ssG )( 151
53
s/
/
D.C gain is 10 and time constant is 3 seconds.
And for following system
D.C Gain of the system is 3/5 and time constant is 1/5
seconds.
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Impulse Response of 1st Order System
Consider the following 1st order system
1Ts
K)(sC)(sR
0t
(t)
1
1 )()( ssR
1Ts
KsC )(
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Impulse Response of 1st Order System
Re-arrange following equation as
1 Ts
KsC )(
TsTKsC/
/)(1
TteT
Ktc /)(
In order represent the response of the system in time domain
we need to compute inverse Laplace transform of the above
equation.
atCe
as
CL
1
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Impulse Response of 1st Order System
Tt
eT
K
tc
/)( IfK=3 and T=2s then
0 2 4 6 8 10
0
0.5
1
1.5
Time
c(t)
K/T*exp(-t/T)
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Step Response of 1st Order System
Consider the following 1st order system
1Ts
K)(sC)(sR
ssUsR 1 )()(
1
Tss
KsC )(
1 Ts
KT
s
KsC )(
In order to find out the inverse Laplace of the above equation, we
need to break it into partial fraction expansion
Forced Response Natural Response
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Step Response of 1st Order System
Taking Inverse Laplace of above equation
1
1
TsT
sKsC )(
TtetuKtc /)()(
Where u(t)=1Tt
eKtc
/)( 1
KeKtc 63201 1 .)(
When t=T
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Step Response of 1st Order System
IfK=10 and T=1.5s thenTteKtc /)( 1
0 1 2 3 4 5 6 7 8 9 100
1
2
3
4
5
6
7
8
9
10
11
Time
c(t)
K*(1-exp(-t/T))
Unit Step Input
Step Response
1
10
Input
outputstatesteadyKGainCD
.
%63
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Step Response of 1st Order System
IfK=10 and T=1, 3, 5, 7TteKtc /)( 1
0 5 10 150
1
2
3
4
5
6
78
9
10
11
Time
c(t)
K*(1-exp(-t/T))
T=3s
T=5s
T=7s
T=1s
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Step Response of 1st order System
System takes five time constants to reach its
final value.
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Step Response of 1st Order System
IfK=1, 3, 5, 10 and T=1TteKtc /)( 1
0 5 10 1
0
1
2
34
5
6
7
8
9
10
11
Time
c(t)
K*(1-exp(-t/T))
K=1
K=3
K=5
K=10
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Relation Between Step and impulse
response
The step response of the first order system is
Differentiating c(t) with respect to t yields
TtTt KeKeKtc //)( 1
Tt
KeKdt
d
dt
tdc /)(
TteT
K
dt
tdc /)(
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Ramp Response of 1st Order System
Consider the following 1st order system
1Ts
K)(sC)(sR
2
1
ssR )(
12 Tss
KsC )(
The ramp response is given as
TtTeTtKtc /)(
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0 5 10 15
0
2
4
6
8
10
Time
c(t)
Unit Ramp Response
Unit Ramp
Ramp Response
Ramp Response of 1st Order System
IfK=1 and T=1Tt
TeTtKtc/
)(
error
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0 5 10 150
2
4
6
8
10
Time
c(t)
Unit Ramp Response
Unit Ramp
Ramp Response
Ramp Response of 1st Order System
IfK=1 and T=3Tt
TeTtKtc
/
)(
error
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Parabolic Response of 1st Order System
Consider the following 1st order system
1Ts
K)(sC)(sR
3
1
ssR )(
13 Tss
KsC )(
Do it yourself
Therefore,
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1st Order System with a Zero
Zero of the system lie at -1/and pole at -1/T.
1
1
Ts
sK
sR
sC )(
)(
)(
11
Tss
sKsC
)()(
Step response of the system would be:
1Ts
TK
s
KsC
)()(
TteTT
KKtc /)()( Tt
eKtc
/
)(
1
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1st Order System with & W/O Zero
1
1
TssK
sRsC )()()(
TteT
T
KKtc /)()( TteKtc /)( 1
1TsK
sRsC)()(
IfT> the response will be same
Tt
enT
K
Ktc/
)()(
TteT
KnKtc /)( 1
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1st Order System with & W/O Zero
IfT> the response of the system would look like
0 5 10 156.5
7
7.5
8
8.5
9
9.5
10
Time
c(t)
Unit Step Response
13
2110
s
s
sR
sC )(
)(
)(
332
3
1010
/)()( tetc
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1st Order System with & W/O Zero
IfT
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1st Order System with a Zero
0 5 10 15
6
7
8
9
10
11
12
13
14
Time
U
nitStepResp
onse
Unit Step Response of 1st Order Systems with Zeros
T
T
t /
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1st Order System with & W/O Zero
0 2 4 6 8 100
2
4
6
8
10
12
14
Time
UnitStepResp
onse
Unit Step Response of 1st Order Systems with Zeros
T
T
1st Order System Without Zero
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Second Order Systems Have discussed the affect of location of poles and zeros on the
transient response of 1st order systems.
Compared to the simplicity of a first-order system, a second-ordersystem exhibits a wide range of responses that must be analyzedand described.
Varying a first-order system's parameter (T, K) simply changes thespeed and offset of the response
Whereas, changes in the parameters of a second-order system can
change theform ofthe response.
A second-order system can display characteristics much like a first-order system or, depending on component values, display dampedorpure oscillations for its transient response.
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Second Order Spring Mass Damper Example
ODE :
Transfer function :
k b
y(t)
F(t)=ku(t)
m
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General Form
A general second-order system is characterized
by the following transfer function.
22
2
2 nn
n
sssR
sC
)(
)(
un-damped natural frequency of the second order system,
which is the frequency of oscillation of the system withoutdamping.
n
damping ratioof the second order system, which is a measure
of the degree of resistance to change in the system output.
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Polar vs. Cartesian representations.Cartesian representation :
Imaginary part (frequency)
Real part (rate of decay)
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Polar vs. Cartesian representations.Cartesian representation :
Imaginary part (frequency)
Real part (rate of decay)
Polar representation :
damping ratio
natural frequency
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Polar vs. Cartesian representations.Cartesian representation :
Imaginary part (frequency)
Real part (rate of decay)
Polar representation :
damping ratio
natural frequency
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Polar vs. Cartesian representations.
Overdamped Critically damped
Underdamped
Undamped
Significance of the damping ratio :
System transfer function :
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Polar vs. Cartesian representations.System transfer function :
Significance of the damping ratio :
Overdamped Critically damped
Underdamped
Undamped
P l C t i t ti
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Polar vs. Cartesian representations.
System transfer function :
Significance of the damping ratio :
Overdamped Critically damped
Underdamped
Undamped
All 4 cases Unless overdamped
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Poles of Second Order System
Pole Locations22
21,2
2 0
( 1)
n n
n n
s s
p
Over damped
(two real distinct roots = two 1st
order systems with real poles)Critically damped
(a single pole of multiplicity two,
highly unlikely, requires exact
matching)
Underdamped
(complex conjugate pair of poles,
oscillatory behavior, most
common)
Real
Im.
n
n
1. If 0 <
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Pole position vs time response
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Pole variation vs time response
TRANSIENT
CHARACTERISITCS AREAFFECTED BY POLE
LOCATIONS
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Definitions of Transient Response Specifications
1. Delay time, : The delay time is the time required for the
response to reach half the final value.
2. Rise time, : The rise time is the time required for the response
to rise from 10% to 90%, 5% to 95%, or 0% to 100% of its final
value. For underdamped second-order systems, the 0% to 100%rise time is normally used. For overdamped systems, the 10% to
90% rise time is commonly used.
3. Peak time, : The peak time is the time required for the
response to reach the first peak of the overshoot.
dt
rt
pt
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Definitions of Transient Response Specifications
4. Maximum (percent) overshoot, : The maximum overshoot is
the maximum peak value of the response curve measured from
unity. If the final steady-state value of the response differs from
unity, then, it is common to use the maximum percent overshoot.
It is defined by
Maximum percent overshoot =
5. Settling time, : The settling time is the time required for the
response curve to reach and stay within a range about the final
value of size specified by absolute percentage of the final value(usually 2% or 5%).
%100)(
)()(
c
ctc p
st
pM
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The system is assumed to be underdamped.
Rise time: Referring to Eq. (5-3), we obtain the rise time by letting
.
Then, we have
rdrd
t
r
ttetc rn
sin
1cos11)(
2
rt
1)( rtc
d
n
nrdt
2211
tan
d
d
drt
1tan
1
Rise Time
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Peak time: Referring to Eq. (5-3), we may obtain the peak time by
differentiating with respect to time and letting this derivative equal to
zero. Since
Then, we have
The last equation yields the following equation:
or
Since the peak time corresponds to the first peak overshoot, Hence
te
ttettedt
dc
d
tn
dd
dd
t
dd
t
n
n
nn
sin
1
cos1
sinsin1
cos
2
22
0sin1 2
pd
tn
tt
tedt
dcpn
p
0sin pdt
Peak Time
,3,2,,0 pdt
dpt
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Maximum overshoot: The maximum overshoot occurs at the peak timeor . It is possible to obtain
The maximum percent overshoot is .
)1/(
2
)/(
2
sin1
cos1)(
e
etcM dnpp
%100)1/( 2
e
Maximum Overshoot
dptt /
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Settling time: For convenience in comparing the responses ofsystems, the settling time is defined to be
or
)criterion%2(44
4n
s Tt
)criterion%5(33
3n
s Tt
Pair of envelope curves forhe unit-step response curve
Settling Time
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Max Overshoot vs curve