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TOPIC :TIME RESPONSE ANALYSIS
GROUP NAME :
1.JAIMIN ATODARIA (150990109001)
2.RAVIRAJ SOLANKI (150990109011)
GUIDED BY : MS. RICHA DUBEY
CONTENT
 Introduction
 Time Response
 Input Supplied System
 Steady State Response and Error
 Types Of The Systems
 Analysis Of First Order System
 Analysis Of Second Order System
 Transient Response specification
 Limitations
 Sums
Introduction
 Time response of the system is defined as the output
of a system when subjected to an input which is a
function of time.
 Time response analysis means subjected the control
system to inputs that are functions of time and
studying their output which are also function of time.
DEFINITIONS
TIME RESPONSE: The time response of a system is the
output (response) which is function of the time, when
input (excitation) is applied.
Time response of a control system consists of two parts
1. Transient Response 2. Steady State Response
Mathematically, c(t)  ct (t)  css (t)
Where, ct (t) = transient response
css (t) = steady stateresponse
TRANSIENT RESPONSE: The transient response is the
part of response which goes to zero as time
increases. Mathematically
Lim ct (t)  0
t
The transient response may be exponential or
oscillatory in nature.
STEADY STATE: The steady state response is the part of
the total response after transient has died.
STEADY STATE ERROR: If the steady state response of
the output does not match with the input then the
system has steady state error, denoted by ess .
TIME RESPONSE
 A control system generates an output or response for
given input.
 The input represents the desired response while the
output is actual response of system.
 Ex. Elevator
 As defined earlier, time response is the response of
control system as a function of time.
TIME RESPONSE
• The time response analysis is
divided into two parts
•i) the output is changing with
respect to time.
(transient response)
•ii) the output is almost constant.
(steady state response)
 So that the total time response, Ct(t) followed by the
steady state response Css(t).
 C(t) = transient + steady state response
 C(t) = Ct(t) + Css(t)
TIME RESPONSE
 For time response analysis of control systems, we need
to subject the system to various test inputs.
 Test input signals are used for testing how well a
system responds to known input.
 Some of standards test signals that are used are:
 Impulse
 Step
 Ramp
 Parabola
 Sinusoidal
INPUT SUPPLIED TO SYSTEM
INPUT SUPPLIED TO SYSTEM
IMPULSE INPUT
•It is sudden change input. An impulse is
infinite at t=0 and everywhere else.
• r(t)= δ(t)= 1 t =0
= 0 t ≠o
In laplase domain we have,
• L[r(t)]= 1
STEP INPUT
•It represents a constant command such
as position. Like elevator is a step input.
•r(t)= u(t)= A t ≥0
= 0 otherwise
L[r(t)]= A/s
RAMP INPUT
• this represents a linearly increasing
input command.
•r(t) = At t ≥0,Aslope
= 0 t <0
L[r(t)]= A/s²
A= 1 then unit ramp
INPUT SUPPLIED TO SYSTEM
PARABOLIC INPUT
•Rate of change of velocity is
acceleration. Acceleration is a parabolic
function.
• r(t) = At ²/2 t ≥0
= 0 t <0
L[r(t)]= A/s³
SINUSOIDAL INPUT
•It input of varying and study the system
frequently response.
• r(t) = A sin(wt) t ≥0
STEADY STATE ERROR:
The steady state error is the difference between the input and
output of the system during steady state.
For accuracy steady state error should be minimum. We know
that
The steady state error of the system is obtained by final value theorem
1
R(s)
1 G(s)H (s)
E(s) 
R(s) 1 G(s)H (s)
E(s)

ss
t s0
e  lime(t)  lims.E(s)
R(s)
ss
ss
1 G(s)
e  lims.
H(s) 1
1 G(s)H (s)
e  lims.
s0
s0
For unity feedback
Thus, the steady state error depends on the input and
open loop transfer function.
R(s)
STATIC ERROR COEFFICIENTS
POSITIONAL ERROR CONSTANT Kp: For unit step
11
1
p
ss
ss
s0
s0
K  limG(s)H(s)
s0
1 Kp

1 limG(s)H(s)
e 
s 1 G(s)H(s)
e  lims.
1
.
Where is the positional error constantKp
input R(s)=1/s
Steady state error
VELOCITY ERROR CONSTANT (Kv):
Steady state error with a unit ramp input is given by R(s)=1/s2
1
ss
1 G(s)H (s)
e  Lims.R(s).
s0
v
ess
ess
1 1
11 1
2
 lim
.  lim
s 1 G(s)H (s)
 lims.
s0 sG(s)H (s) K
s0 s  sG(s)H (s)s0
Where
s0
Kv  limsG(s)H (s) velocity error coefficient
ACCELERATION ERROR CONSTANT (Ka):
The steady state error of the system with unit parabolic input is given
by
where,
a
ess
ess
1 1
11
s3
 lim
 lim
1 G(s)H (s)
R(s) 
1
s0 s2
G(s)H(s) K
s0 s2
 s2
G(s)H (s)
 lim s.
1
.
s0 s3
a
s0
K  lims2
G(s)H (s) acceleration constant.
STEADY STATE ERROR FOR DIFFERENT TYPE OF SYSTEMS
m
s (1 sTa )(1sTb ).........
TYPE 0 SYSTEM WITH UNIT STEP INPUT:
Consider open loop transfer function
G(s)H(s) 
K(1 sT1)(1 sT2 )..........
   (1)
p
ess 
ess 
1 K
1 Kp 1 K
1
1 1
K  limG(s)H (s)  K
R(s) 
1
s
s0 Hence , for type 0 system the
static position error constant Kp
isfinite.
TYPE 0 SYSTEM WITH UNIT RAMP INPUT:
TYPE 0 SYSTEM WITH UNIT PARABOLIC INPUT:
For type ‘zero system’ the steady state error is infinite for ramp and
parabolic inputs. Hence, the ramp and parabolic inputs are not
acceptable.
  
v
Kv
ess
1
(1 sTa )(1sTb )....
K  limsG(s)H (s)  lims.
K(1 sT1)(1 sT2 )...
 0
s0 s0
ess  
a b
a
Ka
1
ess 
(1 sT )(1 sT )....
K  lims2
G(s)H (s)  lims2
.
K(1 sT1)(1 sT2 )...
 0
s0 s0
ess  
TYPE 1 SYSTEM WITH UNIT STEP INPUT:
TYPE 1 SYSTEM WITH UNIT RAMP INPUT:
Put the value of G(s)H(s) from eqn.1
p
s0
K  limG(s)H(s)
ss
1 Kp
e 
1
 0
Put the value of G(s)H(s) from eqn.1
Kp  
ess  0
v
s0
K  lims.G(s)H(s)
Kv K
ess
1

1

Kv  K
ss

1
K
e
TYPE 1 SYSTEM WITH UNIT PARABOLIC INPUT:
Put the value of G(s)H(s) from eqn.1
Hence, it is clear that for type 1 system step input and ramp inputs
are acceptable and parabolic inputis not acceptable.
Similarly we can find for type 2 system.
For type two system all three inputs (step, Ramp, Parabolic) are
acceptable.
a
s0
K  lims2
G(s)H (s)
Ka
ess   
1
Ka  0
ess  
SUMMARY FOR TYPE 0,TYPE 1 &TYPE 2 SYSTEM
INPUT
SIGNALS
TYPE ‘0’
SYSTEM
TYPE ‘1’
SYSTEM
TYPE ‘2’
SYSTEM
UNIT STEP
INPUT
1
1 K 0 0
UNIT RAMP
INPUT 
1
K 0
UNIT
PARABOLIC
INPUT
  1
K
time response analysis
Example: Find Static Error Constants For The Given
System.
EXAMPLE 1: The open loop transfer function of unity
feedback system is given by
SOLUTION:
50
(1 0.1s)(s10)
G(s) 
Determine the static error coefficients Kp ,Kv ,Ka
50
50
50
 0
 0
5 lim
(1 0.1s)(s10)
(1 0.1s)(s10)
K  lims.G(s)H(s)
K  limG(s)H(s)
 lims2
s0
2
Ka  s G(s)H (s)
 lims.
s0
s0
v
s0 (1 0.1s)(s 10)
s0
p
time response analysis
Analysis of first order system for Step input function
Consider a first order system as shown;
+
-
R(s) C(s)
Here and
1
Ts
1
(s)G
Ts
 H(s) 1
C(s)
(s) 1
G
R GH
 

1
1
1
Ts
Ts


1
1 Ts


r(t) = u(t) t>0
= 0 t<0
For step input;
Taking Laplace transform;
but
Analysis of first order system for Step input function
1
(s) {Ru(t)}R L
s
 
(s) 1
(s) 1
C
R Ts


1
(s) (s)
1
C R
Ts
  

Using partial fraction;
Solving;
09/24/2017 Amit Nevase
Conti..
1 1
(s)
1
C
Ts s
  

(s)
1
A B
C
s
s
T
  

0. (s) | 1sA s C   
1
1
( ) (s) | 1
s
T
B s C
T 
    
Taking Inverse Laplace transform;
Conti..
1 1
(s)
1
C
s
s
T
  

1 1 11 1
(t) { (s)} { } { }
1
c L C L L
s
s
T
  
   

1
(t) 1
t
T
c e

  
Plot C(t) vs t;
Sr. No. t C(t)
1 T 0.632
2 2T 0.86
3 3T 0.95
4 4T 0.982
5 5T 0.993
6 1
Analysis of first order system for unit impulse function
Input is unit impulse function R(s)=1
1
1
c(t) 
1
et /T
T
T s 1/T
C(s) 
1
sT 1
C(s)  .1
sT 1
1
C(s)  R(s)
Inverse Laplace transform
Analysis of first order system for unit Ramp function
T
s s
1
1
R(s)
1
2
s2
s 
1
C(s) 
1

T
T
s2
(1 sT)
C(s) 
R(s) 
1
sT 1
C(s) 
R(s) sT 1
C(s)

1
Input is unit Ramp
After partial fraction
We know that
The steady state error is equal to ‘T’, where ‘T’ is the
time constant of the system.
For smaller time constant steady state error will be
small and speed of the response will increase.
t
e(t)  r(t)  c(t)
e(t)  t tT Tet /T

e(t)  T(1 et /T
)
 Limit(T Tet /T
)  T
Take inverse Laplace, we get
c(t)  t T Tet /T
Error signal
Steady state error
time response analysis
Block diagram of second order system is shown in fig.
R(s) C(s)
_
+
2
n
s(s  2n)
n
n
R(s)
R(s) s
R(s) s
2
n
2
2
n
2
n
2
2
n
R(s) 
1
s
C(s)

   (A)
C(s)

 2 s 

 2 s 

For unit step input
2
1
2
nn
n
2
    (1)
s s  2 s 
C(s)  .
Replace s2
 2 s 2
by
n n
(s  )2
2
(12
)
n n
Break the equation by partial fraction and put 2
 2
(12
)
d n
1
.      (3)
A 1
B

A

n d
2
n
s (s  )2
2
n d
s (s  )2
2

2
(2)

n n
n
s (s  )2
2
(12
)
C(s) 
1
.
22
dn (s )Multiply equation (3) by  and put
2
2
(  j )
B  n n d
(n  jd )(n  jd )
 jd  s n
B  (n  s n )  (s  2n )
B  n
 n  jd
B  n
s
s  n  jd
2
Equation (1) can be written as
222 

(4)
 d nd
2
dns
C(s) 
1


C(s) 
1

 (s  )(s  )
n d
s n

n
.
d
s (s  )2
2
s n n
Laplace Inverse of equation (4)
(5)




c(t) 1 e d 

d
nn
e .sin tn
d

.cos t   t t
2
d  n 1Put
e
dd

.cos t2
 sin t1
12
c(t) 1

.sindt
 12

cosdt c(t) 1 e
nt
nt
2
12
1
tan 
12
 sin
cos  
sin( t )

e
c(t) 1 d
nt
Put
    (6)

1 2 
sin(
12
12
)t  tan1e
c(t) 1 n
nt
Put the values ofd & 
    (7)

1  2 
sin(
1  2

1  2
)t  tan1e
e(t)  n
nt
Error signal for the system
e(t)  r(t)  c(t)
The poles are;
(i) Real and Unequal if
i.e. They lie on real axis and distinct
(ii) Real and equal if
i.e. They are repeated on real axis
(iii) Complex if
i.e. Poles are in second and third quadrant
Analysis of second order system for Step input
2
1 0  
1 
2
1 0  
1 
2
1 0  
1 
Relation between and pole locations
(i) Under damped
Pole Location Step Response c(t)

0 1 
(ii) Critically damped
Pole Location Step Response c(t)
Relation between and pole locations
1 

(iii) over damped
Pole Location Step Response c(t)
Relation between and pole locations
1 

(iv)
Pole Location
Relation between and pole locations
0 

TRANSIENT RESPONSE SPECIFICATIONS
 Specifications for a control system design often involve
certain requirements associated with the time
response of the closed-loop system.
 The requirements are specified by the behavior of the
controlled variable or by the control error on well
defined test signals.
 The most important test signal is a unit step on the
input of the control system and requirements are
placed on the behavior of the controlled variable
 The maximum overshoot is the magnitude of the overshoot after
the first crossing of the steady-state value (100%).
 The peak time is the time required to reach the maximum
overshoot.
 The settling time is the time for the controlled variable first to
reach and thereafter remain within a prescribed percentage of
the steady-state value. Common values of are 2%, 3% or 5%.
 The rise time is the time required to reach first the steady-state
value (100%).
TIME RESPONSE SPECIFICATIONS
Time Response Specifications
1. DELAY TIME (td):
It is time required for the response to reach
50% of the final value in the first attempt.
1 0.7
d
n
t




2. RISE TIME (tr): It is time required for the response to
rise from 10% to 90% of its final value for over-
damped systems and 0 to 100% for under-damped
systems.

2
2
1 
1  2
  tan1
sin 1  t  e
We know that:
c(t) 1 n
nt
Where,
Let response reaches 100% of desired value. Put c(t)=1
  
2
2
11 sin
1 12
 1
12
sin t  0
e
t 
e
n
n
nt
nt
 0Since, ent
sin((n
sin((n 12
)t )  sin(n)
12
)t )  0
Or,
Put n=1
2
 12
 
n
tr 
(n 1  )tr    
 12
12
  tan1
 
n
rt
Or,
Or,
3. PEAK TIME (tp): The peak time is the time required
for the response to reach the first peak of the time
response or first peak overshoot.
n
nt
sin 12
t  e
12
c(t) 1Since
For maximum
 0  (1)

n
nn
dt
dc(t)
 0
ent
nt
12
n
12
t 
dc(t) e
dt
sin
1 2
cos 12
t 
12
Since,
Equation can be written as
Equation (2) becomes
 0ent
cos
12
 sin
12
t 12
t 12
 sinnn
Put and   cos
12
t cos12
t sin  sin
n
cosn
cos
sin
cos((
sin((
12
)t )
12
)t )
n
n

tan((n 1 )t )  n
2
(n 1 )tp  n
2
The time to various
peak
Where n=1,2,3,…….
Peak time to first overshoot, put n=1

 12
n
pt
First minimum (undershoot) occurs at n=2
min
2
 12
n
t
4. MAXIMUM OVERSHOOT (MP):
Maximum overshoot occur at peak time, t=tp
in above equation
n
nt
sin 12
t  e
12
c(t) 1

 12
n
pt

Put,





 12

12
.

sin
12
n
n
n 12
n
e
c(t) 1
sin



12
12
12
sin( )
12
12

12

12

c(t)  1
e
e
c(t) 1
e
c(t) 1
Put, sin  12
sin( )  sin



12

12

12

1
M  e
M 1 e
c(t) 1 e
p
p
M p  c(t)1
*100

12

M % ep
time response analysis
5. SETTLING TIME(ts):
The settling time is defined as the time required
for the transient response to reach and stay
within the prescribed percentage error.
t  4T 
4
s
6. STEADY STATE ERROR (ess): It is difference between
actual output and desired output as time ‘t’ tends to
infinity.
ss
e  Limitr(t)c(t)
t
LIMITATIONAS OF TIME DOMAIN
ANALYSIS
 Control system analysis is carried out in either time
domain or frequency domain. The domain of analysis
depends largely on the design requirements.
 he analysis in the frequency domain is very simple and
quick. Stability determination using a frequency
response plot can be done in very quick time with no
effort.
 In time domain analysis, the analysis becomes
cumbersome for systems of high order. In
frequency domain analysis, the order has a little effect
on the time or effort of analysis.
EXAMPLE 1: The open loop transfer function of a servo
system with unity feedback is given by
Determine the damping ratio, undamped natural frequency
of oscillation. What is the percentage overshoot of the
response to a unit step input.
SOLUTION: Given that
Characteristic equation
10
(s  2)(s  5)
G(s) 
10
H(s) 1
(s  2)(s 5)
G(s) 
1 G(s)H (s)  0
10
 01
s2
 7s  20  0
(s  2)(s  5)
Compare with s2
 2 s 2
 0
n n
We get
*1001.92%1(0.7826)2

*0.7826
12

2* *4.472 7
  0.7826
 2
20
 e
20  4.472rad /sec
M p e
n 
n
2n  7 n 4.472rad /sec
  0.7826
M p 1.92%
EXAMPLE 2: A feedback system is described by the
following transfer function
H (s) Ks
The damping factor of the system is 0.8. determine the
overshoot of the system and value of ‘K’.
SOLUTION: We know that
12
G(s) 
s2
 4s 16
s2
 (4 16K)s 16  0
s2
 (4 16K)s 16R(s)
C(s)

1 G(s)H (s)
16
G(s)
R(s)
C(s)

is the characteristic eqn.
nn
2
n
2
Compare with
2
16
s  2 s   0
n  4rad /sec.
2n  416K
2*0.8*4  416K  K  0.15
*1001(0.8)2

M p 1.5%
*100 eM p  e
0.8
12

time response analysis
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time response analysis

  • 1. TOPIC :TIME RESPONSE ANALYSIS GROUP NAME : 1.JAIMIN ATODARIA (150990109001) 2.RAVIRAJ SOLANKI (150990109011) GUIDED BY : MS. RICHA DUBEY
  • 2. CONTENT  Introduction  Time Response  Input Supplied System  Steady State Response and Error  Types Of The Systems  Analysis Of First Order System  Analysis Of Second Order System  Transient Response specification  Limitations  Sums
  • 3. Introduction  Time response of the system is defined as the output of a system when subjected to an input which is a function of time.  Time response analysis means subjected the control system to inputs that are functions of time and studying their output which are also function of time.
  • 4. DEFINITIONS TIME RESPONSE: The time response of a system is the output (response) which is function of the time, when input (excitation) is applied. Time response of a control system consists of two parts 1. Transient Response 2. Steady State Response Mathematically, c(t)  ct (t)  css (t) Where, ct (t) = transient response css (t) = steady stateresponse
  • 5. TRANSIENT RESPONSE: The transient response is the part of response which goes to zero as time increases. Mathematically Lim ct (t)  0 t The transient response may be exponential or oscillatory in nature. STEADY STATE: The steady state response is the part of the total response after transient has died. STEADY STATE ERROR: If the steady state response of the output does not match with the input then the system has steady state error, denoted by ess .
  • 6. TIME RESPONSE  A control system generates an output or response for given input.  The input represents the desired response while the output is actual response of system.  Ex. Elevator
  • 7.  As defined earlier, time response is the response of control system as a function of time. TIME RESPONSE • The time response analysis is divided into two parts •i) the output is changing with respect to time. (transient response) •ii) the output is almost constant. (steady state response)
  • 8.  So that the total time response, Ct(t) followed by the steady state response Css(t).  C(t) = transient + steady state response  C(t) = Ct(t) + Css(t) TIME RESPONSE
  • 9.  For time response analysis of control systems, we need to subject the system to various test inputs.  Test input signals are used for testing how well a system responds to known input.  Some of standards test signals that are used are:  Impulse  Step  Ramp  Parabola  Sinusoidal INPUT SUPPLIED TO SYSTEM
  • 10. INPUT SUPPLIED TO SYSTEM IMPULSE INPUT •It is sudden change input. An impulse is infinite at t=0 and everywhere else. • r(t)= δ(t)= 1 t =0 = 0 t ≠o In laplase domain we have, • L[r(t)]= 1 STEP INPUT •It represents a constant command such as position. Like elevator is a step input. •r(t)= u(t)= A t ≥0 = 0 otherwise L[r(t)]= A/s RAMP INPUT • this represents a linearly increasing input command. •r(t) = At t ≥0,Aslope = 0 t <0 L[r(t)]= A/s² A= 1 then unit ramp
  • 11. INPUT SUPPLIED TO SYSTEM PARABOLIC INPUT •Rate of change of velocity is acceleration. Acceleration is a parabolic function. • r(t) = At ²/2 t ≥0 = 0 t <0 L[r(t)]= A/s³ SINUSOIDAL INPUT •It input of varying and study the system frequently response. • r(t) = A sin(wt) t ≥0
  • 12. STEADY STATE ERROR: The steady state error is the difference between the input and output of the system during steady state. For accuracy steady state error should be minimum. We know that The steady state error of the system is obtained by final value theorem 1 R(s) 1 G(s)H (s) E(s)  R(s) 1 G(s)H (s) E(s)  ss t s0 e  lime(t)  lims.E(s)
  • 13. R(s) ss ss 1 G(s) e  lims. H(s) 1 1 G(s)H (s) e  lims. s0 s0 For unity feedback Thus, the steady state error depends on the input and open loop transfer function. R(s)
  • 14. STATIC ERROR COEFFICIENTS POSITIONAL ERROR CONSTANT Kp: For unit step 11 1 p ss ss s0 s0 K  limG(s)H(s) s0 1 Kp  1 limG(s)H(s) e  s 1 G(s)H(s) e  lims. 1 . Where is the positional error constantKp input R(s)=1/s Steady state error
  • 15. VELOCITY ERROR CONSTANT (Kv): Steady state error with a unit ramp input is given by R(s)=1/s2 1 ss 1 G(s)H (s) e  Lims.R(s). s0 v ess ess 1 1 11 1 2  lim .  lim s 1 G(s)H (s)  lims. s0 sG(s)H (s) K s0 s  sG(s)H (s)s0 Where s0 Kv  limsG(s)H (s) velocity error coefficient
  • 16. ACCELERATION ERROR CONSTANT (Ka): The steady state error of the system with unit parabolic input is given by where, a ess ess 1 1 11 s3  lim  lim 1 G(s)H (s) R(s)  1 s0 s2 G(s)H(s) K s0 s2  s2 G(s)H (s)  lim s. 1 . s0 s3 a s0 K  lims2 G(s)H (s) acceleration constant.
  • 17. STEADY STATE ERROR FOR DIFFERENT TYPE OF SYSTEMS m s (1 sTa )(1sTb )......... TYPE 0 SYSTEM WITH UNIT STEP INPUT: Consider open loop transfer function G(s)H(s)  K(1 sT1)(1 sT2 )..........    (1) p ess  ess  1 K 1 Kp 1 K 1 1 1 K  limG(s)H (s)  K R(s)  1 s s0 Hence , for type 0 system the static position error constant Kp isfinite.
  • 18. TYPE 0 SYSTEM WITH UNIT RAMP INPUT: TYPE 0 SYSTEM WITH UNIT PARABOLIC INPUT: For type ‘zero system’ the steady state error is infinite for ramp and parabolic inputs. Hence, the ramp and parabolic inputs are not acceptable.    v Kv ess 1 (1 sTa )(1sTb ).... K  limsG(s)H (s)  lims. K(1 sT1)(1 sT2 )...  0 s0 s0 ess   a b a Ka 1 ess  (1 sT )(1 sT ).... K  lims2 G(s)H (s)  lims2 . K(1 sT1)(1 sT2 )...  0 s0 s0 ess  
  • 19. TYPE 1 SYSTEM WITH UNIT STEP INPUT: TYPE 1 SYSTEM WITH UNIT RAMP INPUT: Put the value of G(s)H(s) from eqn.1 p s0 K  limG(s)H(s) ss 1 Kp e  1  0 Put the value of G(s)H(s) from eqn.1 Kp   ess  0 v s0 K  lims.G(s)H(s) Kv K ess 1  1  Kv  K ss  1 K e
  • 20. TYPE 1 SYSTEM WITH UNIT PARABOLIC INPUT: Put the value of G(s)H(s) from eqn.1 Hence, it is clear that for type 1 system step input and ramp inputs are acceptable and parabolic inputis not acceptable. Similarly we can find for type 2 system. For type two system all three inputs (step, Ramp, Parabolic) are acceptable. a s0 K  lims2 G(s)H (s) Ka ess    1 Ka  0 ess  
  • 21. SUMMARY FOR TYPE 0,TYPE 1 &TYPE 2 SYSTEM INPUT SIGNALS TYPE ‘0’ SYSTEM TYPE ‘1’ SYSTEM TYPE ‘2’ SYSTEM UNIT STEP INPUT 1 1 K 0 0 UNIT RAMP INPUT  1 K 0 UNIT PARABOLIC INPUT   1 K
  • 23. Example: Find Static Error Constants For The Given System.
  • 24. EXAMPLE 1: The open loop transfer function of unity feedback system is given by SOLUTION: 50 (1 0.1s)(s10) G(s)  Determine the static error coefficients Kp ,Kv ,Ka 50 50 50  0  0 5 lim (1 0.1s)(s10) (1 0.1s)(s10) K  lims.G(s)H(s) K  limG(s)H(s)  lims2 s0 2 Ka  s G(s)H (s)  lims. s0 s0 v s0 (1 0.1s)(s 10) s0 p
  • 26. Analysis of first order system for Step input function Consider a first order system as shown; + - R(s) C(s) Here and 1 Ts 1 (s)G Ts  H(s) 1 C(s) (s) 1 G R GH    1 1 1 Ts Ts   1 1 Ts  
  • 27. r(t) = u(t) t>0 = 0 t<0 For step input; Taking Laplace transform; but Analysis of first order system for Step input function 1 (s) {Ru(t)}R L s   (s) 1 (s) 1 C R Ts   1 (s) (s) 1 C R Ts    
  • 28. Using partial fraction; Solving; 09/24/2017 Amit Nevase Conti.. 1 1 (s) 1 C Ts s     (s) 1 A B C s s T     0. (s) | 1sA s C    1 1 ( ) (s) | 1 s T B s C T      
  • 29. Taking Inverse Laplace transform; Conti.. 1 1 (s) 1 C s s T     1 1 11 1 (t) { (s)} { } { } 1 c L C L L s s T         1 (t) 1 t T c e    
  • 30. Plot C(t) vs t; Sr. No. t C(t) 1 T 0.632 2 2T 0.86 3 3T 0.95 4 4T 0.982 5 5T 0.993 6 1
  • 31. Analysis of first order system for unit impulse function Input is unit impulse function R(s)=1 1 1 c(t)  1 et /T T T s 1/T C(s)  1 sT 1 C(s)  .1 sT 1 1 C(s)  R(s) Inverse Laplace transform
  • 32. Analysis of first order system for unit Ramp function T s s 1 1 R(s) 1 2 s2 s  1 C(s)  1  T T s2 (1 sT) C(s)  R(s)  1 sT 1 C(s)  R(s) sT 1 C(s)  1 Input is unit Ramp After partial fraction We know that
  • 33. The steady state error is equal to ‘T’, where ‘T’ is the time constant of the system. For smaller time constant steady state error will be small and speed of the response will increase. t e(t)  r(t)  c(t) e(t)  t tT Tet /T  e(t)  T(1 et /T )  Limit(T Tet /T )  T Take inverse Laplace, we get c(t)  t T Tet /T Error signal Steady state error
  • 35. Block diagram of second order system is shown in fig. R(s) C(s) _ + 2 n s(s  2n) n n R(s) R(s) s R(s) s 2 n 2 2 n 2 n 2 2 n R(s)  1 s C(s)     (A) C(s)   2 s    2 s   For unit step input
  • 36. 2 1 2 nn n 2     (1) s s  2 s  C(s)  . Replace s2  2 s 2 by n n (s  )2 2 (12 ) n n Break the equation by partial fraction and put 2  2 (12 ) d n 1 .      (3) A 1 B  A  n d 2 n s (s  )2 2 n d s (s  )2 2  2 (2)  n n n s (s  )2 2 (12 ) C(s)  1 .
  • 37. 22 dn (s )Multiply equation (3) by  and put 2 2 (  j ) B  n n d (n  jd )(n  jd )  jd  s n B  (n  s n )  (s  2n ) B  n  n  jd B  n s s  n  jd 2
  • 38. Equation (1) can be written as 222   (4)  d nd 2 dns C(s)  1   C(s)  1   (s  )(s  ) n d s n  n . d s (s  )2 2 s n n Laplace Inverse of equation (4) (5)     c(t) 1 e d   d nn e .sin tn d  .cos t   t t 2 d  n 1Put
  • 39. e dd  .cos t2  sin t1 12 c(t) 1  .sindt  12  cosdt c(t) 1 e nt nt 2 12 1 tan  12  sin cos   sin( t )  e c(t) 1 d nt Put
  • 40.     (6)  1 2  sin( 12 12 )t  tan1e c(t) 1 n nt Put the values ofd &      (7)  1  2  sin( 1  2  1  2 )t  tan1e e(t)  n nt Error signal for the system e(t)  r(t)  c(t)
  • 41. The poles are; (i) Real and Unequal if i.e. They lie on real axis and distinct (ii) Real and equal if i.e. They are repeated on real axis (iii) Complex if i.e. Poles are in second and third quadrant Analysis of second order system for Step input 2 1 0   1  2 1 0   1  2 1 0   1 
  • 42. Relation between and pole locations (i) Under damped Pole Location Step Response c(t)  0 1 
  • 43. (ii) Critically damped Pole Location Step Response c(t) Relation between and pole locations 1  
  • 44. (iii) over damped Pole Location Step Response c(t) Relation between and pole locations 1  
  • 45. (iv) Pole Location Relation between and pole locations 0  
  • 46. TRANSIENT RESPONSE SPECIFICATIONS  Specifications for a control system design often involve certain requirements associated with the time response of the closed-loop system.  The requirements are specified by the behavior of the controlled variable or by the control error on well defined test signals.  The most important test signal is a unit step on the input of the control system and requirements are placed on the behavior of the controlled variable
  • 47.  The maximum overshoot is the magnitude of the overshoot after the first crossing of the steady-state value (100%).  The peak time is the time required to reach the maximum overshoot.  The settling time is the time for the controlled variable first to reach and thereafter remain within a prescribed percentage of the steady-state value. Common values of are 2%, 3% or 5%.  The rise time is the time required to reach first the steady-state value (100%). TIME RESPONSE SPECIFICATIONS
  • 49. 1. DELAY TIME (td): It is time required for the response to reach 50% of the final value in the first attempt. 1 0.7 d n t    
  • 50. 2. RISE TIME (tr): It is time required for the response to rise from 10% to 90% of its final value for over- damped systems and 0 to 100% for under-damped systems.  2 2 1  1  2   tan1 sin 1  t  e We know that: c(t) 1 n nt Where,
  • 51. Let response reaches 100% of desired value. Put c(t)=1    2 2 11 sin 1 12  1 12 sin t  0 e t  e n n nt nt  0Since, ent sin((n sin((n 12 )t )  sin(n) 12 )t )  0 Or, Put n=1
  • 52. 2  12   n tr  (n 1  )tr      12 12   tan1   n rt Or, Or,
  • 53. 3. PEAK TIME (tp): The peak time is the time required for the response to reach the first peak of the time response or first peak overshoot. n nt sin 12 t  e 12 c(t) 1Since For maximum  0  (1)  n nn dt dc(t)  0 ent nt 12 n 12 t  dc(t) e dt sin 1 2 cos 12 t  12
  • 54. Since, Equation can be written as Equation (2) becomes  0ent cos 12  sin 12 t 12 t 12  sinnn Put and   cos 12 t cos12 t sin  sin n cosn cos sin cos(( sin(( 12 )t ) 12 )t ) n n 
  • 55. tan((n 1 )t )  n 2 (n 1 )tp  n 2 The time to various peak Where n=1,2,3,……. Peak time to first overshoot, put n=1   12 n pt First minimum (undershoot) occurs at n=2 min 2  12 n t
  • 56. 4. MAXIMUM OVERSHOOT (MP): Maximum overshoot occur at peak time, t=tp in above equation n nt sin 12 t  e 12 c(t) 1   12 n pt  Put,       12  12 .  sin 12 n n n 12 n e c(t) 1
  • 57. sin    12 12 12 sin( ) 12 12  12  12  c(t)  1 e e c(t) 1 e c(t) 1 Put, sin  12 sin( )  sin
  • 58.    12  12  12  1 M  e M 1 e c(t) 1 e p p M p  c(t)1 *100  12  M % ep
  • 60. 5. SETTLING TIME(ts): The settling time is defined as the time required for the transient response to reach and stay within the prescribed percentage error. t  4T  4 s
  • 61. 6. STEADY STATE ERROR (ess): It is difference between actual output and desired output as time ‘t’ tends to infinity. ss e  Limitr(t)c(t) t
  • 62. LIMITATIONAS OF TIME DOMAIN ANALYSIS  Control system analysis is carried out in either time domain or frequency domain. The domain of analysis depends largely on the design requirements.  he analysis in the frequency domain is very simple and quick. Stability determination using a frequency response plot can be done in very quick time with no effort.  In time domain analysis, the analysis becomes cumbersome for systems of high order. In frequency domain analysis, the order has a little effect on the time or effort of analysis.
  • 63. EXAMPLE 1: The open loop transfer function of a servo system with unity feedback is given by Determine the damping ratio, undamped natural frequency of oscillation. What is the percentage overshoot of the response to a unit step input. SOLUTION: Given that Characteristic equation 10 (s  2)(s  5) G(s)  10 H(s) 1 (s  2)(s 5) G(s)  1 G(s)H (s)  0
  • 64. 10  01 s2  7s  20  0 (s  2)(s  5) Compare with s2  2 s 2  0 n n We get *1001.92%1(0.7826)2  *0.7826 12  2* *4.472 7   0.7826  2 20  e 20  4.472rad /sec M p e n  n 2n  7 n 4.472rad /sec   0.7826 M p 1.92%
  • 65. EXAMPLE 2: A feedback system is described by the following transfer function H (s) Ks The damping factor of the system is 0.8. determine the overshoot of the system and value of ‘K’. SOLUTION: We know that 12 G(s)  s2  4s 16 s2  (4 16K)s 16  0 s2  (4 16K)s 16R(s) C(s)  1 G(s)H (s) 16 G(s) R(s) C(s)  is the characteristic eqn.
  • 66. nn 2 n 2 Compare with 2 16 s  2 s   0 n  4rad /sec. 2n  416K 2*0.8*4  416K  K  0.15 *1001(0.8)2  M p 1.5% *100 eM p  e 0.8 12 
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