Bode Diagram of a Second Order System: Analysis and Interpretation - Prof. Craig A. Woolse, Study notes of Aerospace Engineering

A step-by-step solution to sketch the bode diagram for a given transfer function g(s) = s² + 101s + 100. How to find the zeros and poles, rewrite the transfer function in terms of first order terms, and analyze the magnitude and phase plots for each term. The document also discusses the significance of the resonance peak and the effect of damping ratio on the bode diagram.

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Uploaded on 02/13/2009

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Worked Bode Diagram Example
Problem. Sketch the Bode diagram for the following transfer function:
G(s) = s2+ 101s+ 100
s2+ 4s+ 100 .
Solution. First, compute the zeros and poles. Using the quadratic equation, the zeros are:
z1,2=1
2³101 ±p(101)24(100)´=1,100
Since these roots are both real, we may rewrite the numerator polynomial as a product of first order terms:
s2+ 101s+ 100 = (s+ 1)(s+ 100) = 1
100 ³(s+ 1) ³s
100 + 1´´
The poles are:
p1,2=1
2³4±p(424(100)´.
Since these form a complex conjugate pair, we leave the denominator expression as a quadratic form, but
rewrite it in the following form:
s2+ 4s+ 100 = s2+ 2(0.2)(10)s+ (10)2
= 100 µ³s
10´2
+ 2(0.2) ³s
10´+ 1
Here, we have recognized that the natural frequency and damping ratio associated with the complex
conjugate pair are
ωn= 10 and ζ= 0.2.
We may rewrite G(s) as
G(s) = (s+ 1) ¡s
100 + 1¢
¡s
10 ¢2+ 2(0.2) ¡s
10 ¢+ 1.
Since the system has a unity DC gain, the Bode diagram will be the sum of the Bode diagrams for the
terms
( + 1) ,µ
100 + 1,and 1
³
10 ´2
+ 2(0.2) ³
10 ´+ 1
.
Consider the magnitude plot (in decibels) for the first term: s+ 1. It has a low frequency asymptote of zero
decibels and a high frequency asymptote with a slope of 20 decibels per decade. The asymptotes intersect
at the corner frequency ω= 1 radian per second. The phase at low frequency is zero and the phase at
high frequency is 90. The phase passes through 45at the corner frequency. The second term
100 + 1 has
identical characteristics, except that the corner frequency isω= 100 radians per second.
The third term 1
³
10 ´2
+ 2(0.2) ³
10 ´+ 1
.
represents a complex conjugate pair of poles with damping ratio ζ= 0.2 and natural frequency ωn= 10
radians per second. This term exhibits a low frequency asymptote of zero decibels per decade and a high
frequency asymptote of negative 40 decibels per decade. Because the damping ratio is less than 2
2, there
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Worked Bode Diagram Example

Problem. Sketch the Bode diagram for the following transfer function:

G(s) = s^2 + 101s + 100 s^2 + 4s + 100

Solution. First, compute the zeros and poles. Using the quadratic equation, the zeros are:

z 1 , 2 =

(101)^2 − 4(100)

Since these roots are both real, we may rewrite the numerator polynomial as a product of first order terms:

s^2 + 101s + 100 = (s + 1)(s + 100) =

(s + 1)

( (^) s 100

The poles are:

p 1 , 2 =

(4^2 − 4(100)

Since these form a complex conjugate pair, we leave the denominator expression as a quadratic form, but rewrite it in the following form:

s^2 + 4s + 100 = s^2 + 2(0.2)(10)s + (10)^2

= 100

s 10

( (^) s 10

Here, we have recognized that the natural frequency and damping ratio associated with the complex conjugate pair are ωn = 10 and ζ = 0. 2.

We may rewrite G(s) as

G(s) =

(s + 1)

( (^) s 100 + 1

( (^) s 10

( (^) s 10

Since the system has a unity DC gain, the Bode diagram will be the sum of the Bode diagrams for the terms

(jω + 1) ,

jω 100

, and

jω 10

jω 10

Consider the magnitude plot (in decibels) for the first term: s + 1. It has a low frequency asymptote of zero decibels and a high frequency asymptote with a slope of 20 decibels per decade. The asymptotes intersect at the corner frequency ω = 1 radian per second. The phase at low frequency is zero and the phase at high frequency is 90◦. The phase passes through 45◦^ at the corner frequency. The second term 100 jω + 1 has identical characteristics, except that the corner frequency isω = 100 radians per second.

The third term 1 ( jω 10

jω 10

represents a complex conjugate pair of poles with damping ratio ζ = 0.2 and natural frequency ωn = 10 radians per second. This term exhibits a low frequency asymptote of zero decibels per decade and a high frequency asymptote of negative 40 decibels per decade. Because the damping ratio is less than

√ 2 2 , there

0

50

100

Magnitude (dB)

10 − 10 − 10 0 10 1 10 2 10 3 10 4 −

0

45

90

Phase (deg)

Bode Diagram

Frequency (rad/sec)

Figure 1: Bode diagrams of all three terms.

is a resonance peak just below the corner frequency at ωn. (The smaller the damping ratio, the larger the resonance peak.) There is also a rapid shift from the low frequency phase of zero to the high frequency phase of − 180 ◦. See Figure 1.Summing the three contributions (magnitude and phase) gives the Bode diagram shown in Figure 2.