Bode plot

Ramaiahsubasri 425 views 33 slides Aug 26, 2020
Slide 1
Slide 1 of 33
Slide 1
1
Slide 2
2
Slide 3
3
Slide 4
4
Slide 5
5
Slide 6
6
Slide 7
7
Slide 8
8
Slide 9
9
Slide 10
10
Slide 11
11
Slide 12
12
Slide 13
13
Slide 14
14
Slide 15
15
Slide 16
16
Slide 17
17
Slide 18
18
Slide 19
19
Slide 20
20
Slide 21
21
Slide 22
22
Slide 23
23
Slide 24
24
Slide 25
25
Slide 26
26
Slide 27
27
Slide 28
28
Slide 29
29
Slide 30
30
Slide 31
31
Slide 32
32
Slide 33
33

About This Presentation

Frequency response -plot


Slide Content

BODE PLOT
Dr.R.Subasri
Professor, Kongu Engineering College,
Perundurai, Erode, Tamilnadu, INDIA
1Dr.R.Subasri,KEC,INDIA

2
Frequency Response Techniques
•Analysing the system on frequency basis
e.g communication systems
•Developed by Nyquist and Bode in 1930
•Older than root locus method given by
Evan in 1948
Dr.R.Subasri,KEC,INDIA

3
Frequency Response Techniques
–Radio telescopes used for deep space
communication require precise positioning to
function effectively. To achieve a high degree
of precision ,an accurate mathematical model
of antenna dynamics is to used.
–To construct the model, engineers can test
the antenna by vibrating it with sinusoidal
forces of different frequencies and measuring
the vibrations. These measurements form the
basis for the model.
Dr.R.Subasri,KEC,INDIA

4
Chapter objectives
•Definition of frequency response
•How to plot frequency response
•How to use frequency response to analyse
stability
•How to use frequency response to design
the gain to meet stability specifications.
Dr.R.Subasri,KEC,INDIA

5
Frequency Response Techniques
-Advantages
•modelling transfer functions from physical
data.
•Designing compensators to meet steady
state error and transient response
requirements.
•Finding stability of systems
Dr.R.Subasri,KEC,INDIA

6
Frequency Response
•In the steady state,
sinusoidal inputs to a
linear system
generate sinusoidal
responses of the
same frequency.
•But output differs in
amplitudes and phase
angle from the input
•Differences are
function of frequency.
Dr.R.Subasri,KEC,INDIA

7
Frequency Response)(
)(
)(



i
o
M
M
M = )()()( 
io
−= )()(M )()( 
ii
M  )()( 
oo
M  )()( 
oo
M 
= )]()([)()(  +
i
M
i
M
Magnitude frequency response =
Phase frequency response =
Combination of magnitude and phase frequency responses is Frequency
response
In general Frequency response of a system with transfer function G(s) is )()(M 

jS
sGjG

= /)()(
Dr.R.Subasri,KEC,INDIA

8
Frequency response plots
❖Bode plot(or)Asymptotic
Approximation Plot (or)Logarithmic
plot
❖Polar plot –Nyquist plot
❖Log Magnitude Vs phase angle
Dr.R.Subasri,KEC,INDIA

9
Logarithmic Frequency Scales
On a logarithmic scale, the variable is multiplied by a
given factor for equal increments of length along the
axis.
Decade Change –log
10
Octave change –log
2
Dr.R.Subasri,KEC,INDIA

10
Bode Plot
•Factors of a transfer function
•Constant term K
•-Pure Differentiator-zero at origin -s
-Pure Integrator –pole at origin-1/s
•First order terms
-zero at real axis1+s
-pole at real axis1/1+s
•Second order terms
-complex zero s
2
+2
ns+
n
2
-complex pole 1/ s
2
+2
ns+
n
2
Dr.R.Subasri,KEC,INDIA

11
Constant Kconsatnt factor G(s) = K
-20
0
20
40
0.1 1 10 100
log w
magnitude in db consatnt factor G(s) = K
-90
-45
0
45
90
0.1 1 10 100
log w
phase angle in deg
Magnitude plot is constant and independent of frequency
Phase plot is constant at zero and independent of
frequency
Dr.R.Subasri,KEC,INDIA

12
Pure Integrator 1/spure integrator-pole at origin G(s)=1/s
-40
-20
0
20
40
0.1 1 10 100
logw
mag in db Pure Integrator G(s) = 1 / s
-180
-135
-90
-45
0
45
90
0.1 1 10 100
log w
phase angle in deg
starting point of magnitude plot is -20 log , where is
the starting frequency in the plot. The plot starts from that
point and has the slope of -20 db / dec.
Phase angle is -90-a straight line with no slope
Dr.R.Subasri,KEC,INDIA

13
Pure Differentiator-spure differentiator-zero at origin G(s)=s
-40
-20
0
20
40
0.1 1 10 100
logw
mag in db Pure Differentiator G(s) = s
-90
-45
0
45
90
135
180
0.1 1 10 100
log w
phase angle in deg
starting point of magnitude plot is + 20 log , where is
the starting frequency in the plot. The plot starts from
that point and has the slope of + 20 db / dec.
Phase angle is + 90-a straight line with no slope
Dr.R.Subasri,KEC,INDIA

14
Zero at real axis -1+sfirst order term-zero at real axis
G(s)=1+sT
-40
-20
0
20
40
0.1/T 1/T 10/T 100/T
logwT
mag in db First order term-zero at real axis G(s)=1+sT
-90
-45
0
45
90
135
180
0.1/T 1/T 10/T 100/T
log wT
phase angle in deg
For a constant zero at real axis, in low frequency region, phase angle
is 0and in high frequency region, phase angle is + 90,in between the
slope is + 45/ dec.
For a constant zero at real axis, find the corner frequency 
c= 1/T.Up
to 
c,the magnitude plot is a straight line at 0 db and beyond c, the
plot has a line of slope + 20 db / dec.
Dr.R.Subasri,KEC,INDIA

15
Pole at real axis -1/s+T
For a constant pole at real axis, in low frequency region, phase angle is
0and in high frequency region, phase angle is -90,in between the
slope is -45/ dec.
For a constant zero at real axis, find the corner frequency 
c= T. Up to
c,the magnitude plot is a straight line at 0 db and beyond c, the plot
has a line of slope -20 db / dec.
Dr.R.Subasri,KEC,INDIA

16
Complex zero -s
2
+2
ns+
n
2second order term- complex zero
-40
-20
0
20
40
60
80
100
0.1 1 10 100
log w
mag in db second order term- complex zero
-180
-135
-90
-45
0
45
90
135
180
0.1 1 10 100
log w
phase angle in deg
For a complex zero, find the corner frequency 
c=
n .Up to 
c,the
magnitude plot is a straight line at +40 log 
nand beyond 
c, the plot
has a line of slope + 40 db / dec.
For a complex zero, in low frequency region, phase angle is 0and in
high frequency region, phase angle is + 180,in between the slope is
+ 90/ dec. Dr.R.Subasri,KEC,INDIA

17
Complex pole -1/ s
2
+2
ns+
n
2second order term- complex pole
-100
-80
-60
-40
-20
0
20
40
0.1 1 10 100
log w
mag in db second order term- complex pole
-180
-135
-90
-45
0
45
90
135
180
0.1 1 10 100
log w
phase angle in deg
For a complex pole,find the corner frequency 
c=
n.Up to 
c,the
magnitude plot is a straight line at -40 log 
nand beyond 
c, the plot has
a line of slope -40 db / dec.
For a complex zero, in low frequency region, phase angle is 0and in
high frequency region, phase angle is -180,in between the slope is
-90/ dec.
Dr.R.Subasri,KEC,INDIA

18
Bode Magnitude plot
•For a constant K, magnitude in db is 20
log K-a straight line with no slope
•For a zero at origin or a pole at origin,(s or
1/s) starting point of magnitude plot is 20
log , where is the starting frequency in
the plot. The plot starts from that point and
has the slope of 20 db / dec.
Dr.R.Subasri,KEC,INDIA

19
Bode Magnitude plot
• For a constant zero at real axis or a pole at
real axis(s+T or 1 / s=T),find the corner
frequency 
c= T.
Up to 
c,the magnitude plot is a straight line
at 0 db and beyond c, the plot has a line of
slope 20 db / dec.
•For a complex zero or pole in the form
s
2
+2
ns+
n
2
, find the corner frequency 
c=n.
Up to c,the magnitude plot is a straight line at
40 log 
nand beyond 
c, the plot has a line of
slope 40 db / dec.
Dr.R.Subasri,KEC,INDIA

20
Bode Phase plot
•For a constant K, Phase angle is 0-a
straight line with no slope
•For a zero at origin or a pole at origin,(s or
1/s)-Phase angle is 90-a straight line
with no slope
•For a constant zero at real axis or a pole
at real axis(s+T or 1 / s+T), in low
frequency region, phase angle is 0and in
high frequency region, phase angle is 
90,in between the slope is 45/ dec.
Dr.R.Subasri,KEC,INDIA

21
Bode Phase plot
•For a complex zero or pole, in low
frequency region, phase angle is 0and in
high frequency region, phase angle is 
180,in between the slope is 90/ dec.
•Low frequency region -the frequencies up
to one decade below the corner frequency
•High frequency region -all the frequencies
beyond one decade above the corner
frequency
Dr.R.Subasri,KEC,INDIA

22
Starting point in Bode Plot
Magnitude plot
•Sum of the contributions of
•1. Constant term K ------------20 log K
•2. Zero or pole at origin---------20 log ,
where is the starting frequency in the plot
•3.real zero or pole --------------20 log T
•3. Complex zero or pole--------40 log 
n
Phase plot
Contribution from
•zero at origin or a pole at origin,(s or 1/s) which
is 90.
Dr.R.Subasri,KEC,INDIA

23
Bode magnitude Plot-Example
G(s) = 2s/(s+1)(s+10)
Factor Corner frequency

c
Magnitude in
db
slope
2 -- 20 log 2 -
s - 20 log  20 db / dec
1/1+s 1 Up to =1,20
log1=0 db& 0
slope
Beyond =1,-
20 db / dec
+20 –20 =
0 db / dec.
1 /s+10 10 Up to =10, -
20 log 10 db
& 0 slope
Beyond =10,-
20 db / dec
0 –20 =
-20 db /dec
Dr.R.Subasri,KEC,INDIA

24
Bode magnitude Plot-ExampleMagnitude plot
-40
-20
0
20
40
0.01 0.1 1 10 100
log w
mag in db
Let the starting frequency = 0.1, then starting point of the
plot is:20 log 2 + 20 log 0.1-20 log1-20 log 10= -34 dbDr.R.Subasri,KEC,INDIA

25
40db/dec
20db/dec
-20db/dec
45/dec
90/dec
Dr.R.Subasri,KEC,INDIA

26Dr.R.Subasri,KEC,INDIA

27
Phase plot –slope contribution
Start of
1/1+s
Start of 1
/1+s/10
End of
1/1+s
End of 1
/1+s/10
 0.1 1 10 100
1/1+s-45 -45 - -
1
/1+s/10
- -45 -45 -
Total
slope
-45/ dec-90/ dec-45/ dec-
Dr.R.Subasri,KEC,INDIA

28
Phase plot
The system has one zero at origin, plot starts at +90. Phase plot
-180
-135
-90
-45
0
45
90
135
180
0.010.1 1 10 1001000
log w
phase angle
Dr.R.Subasri,KEC,INDIA

29
Plot to transfer functionMagnitude plot
-12
-8
-4
0
1 2.5 10 25 50
log w
mag in db
Change in magnitude in db(y axis) = slope x
difference in frequency (x axis)
Dr.R.Subasri,KEC,INDIA

30
Plot to transfer function
•Step 1:
Change in magnitude in db= -20 x (log 2.5 –log 1)
= -7.95
= -12 + starting db(y axis)
Starting db= -4.05db
•Step 2:
From the starting point ,there is a slope of -20 db/ dec,
hence there is a pole at origin
Starting db= 20 log K -20 log 
At =1,
-4.05 = 20 log K -20 log 1+20 log 2.5+20 log 10-20 log
25
K=0.627 Dr.R.Subasri,KEC,INDIA

31
Plot to transfer function
•Step 3:
First corner frequency is 2.5
Beyond =2.5 , the slope is changed from -20 db/ dec
to zero db/ dec, hence there should be a zeroat 2.5
Factor is s+ 2.5
•Step 4:
Second corner frequency is 10
Beyond =10 , the slope is changed from 0 db/ decto
+20 db/ dec, hence there should be a zeroat 10
Factor is s+ 10
•Step 3:
Third corner frequency is 25
Beyond =25, the slope is changed from= 20 db/ decto
0 db/ dec, hence there should be a poleat 25
Factor is 1/s+25
0.627(s+2.5) (s+10)/s (s+25)
Dr.R.Subasri,KEC,INDIA

Dr.R.Subasri,KEC,INDIA 32

Thank you
Dr.R.Subasri,KEC,INDIA 33
Tags