linear control system(week-5)
TRANSCRIPT
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7/28/2019 Linear Control System(Week-5)
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Chapter-4 HW Exercises at the End
EL322near
Controlystems
Week-05
12th Mar 17th Mar 2012
Time Response (Contd. )
Chapter#04
Instructor: Engr. Shiraz Latif/ Engr. Atif Fareed/ EngrAreeb Ahmed
nd
Two Important quantities for 2nd order systems Natural Frequency n
The frequency of the oscillations of the system withoutdamping.
Damping Ratio
Ratio of exponential decay frequency to natural frequency
= exponential decay freq / natural freq (rad/sec)
&
Compare both these TF and get the formula for &n
Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
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Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
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.
To analyze the step response ofunderdamped 2nd order systems.
Objectives: To define the transient s ecifications
associated with underdamped responses.
Relate these specifications to pole location,drawing an association between polelocation and response form.
Tie the pole location to system parameters.7Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
General 2nd order sys:
For underdamped response, = ? ?
.
With step input,
Applying Partial fraction
Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
Relationship between value ofand type of response
oscillations
Natural frequency dont cause any affect on the nature of the responseut is on y t e time sca e actor
econ or er un er ampe response orvarying values
9Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
Rise Time: Tr: Time required for the wave form to go from 10% of thefinal value to 90% of the final value.
Peak time: Tp : Time required to reach the first, or maximum, peak
Percentage Overshoot: %OS: The amount that the waveformovershoots thestead state orf inal valueat the eak time ex ressedas a
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p
n
=
percentage of the steady-state value.
Settling time: Ts: Time required for the transients damped oscillations toreach and stay within 2% of the steady state value
1Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
Tr, Tp and Ts yields information about the speed of transient response.
s, r ave same e initions as in irst or er systems.
Same definition for order >2 as well.
These specifications (Tp, Tr, Ts)=
n. Tr
.
No precise expression exists for
Tr but can be obtained from plot & table Normalized rise time = n . Tr
11Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed 1Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
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If location of pole is s; S can be represented as s = d + j d
d is the real part of s exponential damping freq.
d is the imaginary part damped freq of oscillation
Tp, Ts and %OS can berelated to the location of
13Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
Tp is inversely proportion to theimaginary part of the pole
Consider the s-plane
l l l l(same y-value) constant Tp called lines ofconstant peak time
Ts is inversely proportion to the real part
Consider the s-plane
Vertical lines constant real part (same x-value) constant Ts called lines of constant
ll
Radial lines are lines of constant called lines of constant
1Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
%OS
Effect of movement of poles
15Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed
Poles moves verticallyup
Real part same
Pole f butenvelop same
Ts remains same
Poles moveshorizontally left
Imaginary part same
Pole f same ,
damp rapidly
Poles moves atconstant angle (radiallines)
%OS remains same .
Pole away from originhave fast response.
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..
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2)(
2++
+=
ss
ssG
Num = [1 2];
Den = [1 5 3];
T = tf(num,den)
Zeros(T)Implement same
Pzmap(T)
Step (T)
19Instructor:Shiraz Latif/ Atif Fareed/ Areeb Ahmed Grid
xercises
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so p o e s ep response usng
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Transfer function shown above
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