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Reminder: •HW11 due Thursday Lecture: 2nd-order systems...

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Lecture 27: Tue Nov 17, 2020 Reminder: HW11 due Thursday Lecture: 2nd-order systems frequency-domain characteristics three frequencies: natural, resonant, damped
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Page 1: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

0

Lecture 27: Tue Nov 17, 2020

Reminder:

• HW11 due Thursday

Lecture: 2nd-order systems

• frequency-domain characteristics

three frequencies: natural, resonant, damped

Page 2: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Quiz 2 Results

Page 3: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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3084 Reading

Page 4: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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A 2nd-Order System

[ under- ][ critically ][ over- ] damped?

Page 5: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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A 2nd-Order System

[ under- ][ critically ][ over- ] damped?

Page 6: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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A 2nd-Order System

[ under- ][ critically ][ over- ] damped?

Page 7: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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A 2nd-Order System

radius r =

n

Page 8: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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A 2nd-Order System

radius n

let = cos

Page 9: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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A 2nd-Order System

n 1 2–

–n let = cos

radius n

Page 10: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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A 2nd-Order System

n

p1,2 = –n ± jn 1 2–

1 2–

–n let = cos

radius n

⇒ denominator = (s – p1)(s – p2)

= s2 + 2ns + n2

Page 11: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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2nd-Order System: Standard FormGet in the habit — whenever possible, put denominator in “standard form”:

where

• n = “natural” frequency > 0

• = damping coefficient ∈[0, ∞)

• H( 0 ) = H0 = dc gain

H0n2

s2 2n s n2+ +

-----------------------------------------------H( s ) =

Page 12: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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What Kind of Filters are These?

H0n2

s2 2ns n2+ +

-------------------------------------------- Hn 2n s

s2 2n s n2+ +

-------------------------------------------- H∞ s2

s2 2n s n2+ +

--------------------------------------------

Page 13: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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What Kind of Filters are These?

H0n2

s2 2ns n2+ +

-------------------------------------------- Hn 2n s

s2 2n s n2+ +

-------------------------------------------- H∞ s2

s2 2n s n2+ +

--------------------------------------------

HLPF( s ) HBPF( s ) HHPF( s )

0

1

2

3

n 2n

0

1

0

1

2

3

n 2n n 2n

= 0.2

0.3

0.7

0.7

0.2

= 0.2

0.7

0.3

Page 14: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Recall Example

H( s ) = = 48

s2 2s 16+ +-------------------------------- H0n

2

s2 2n s n2+ +

-----------------------------------------------H0 = 3n = 4 = 0.25

½where

|H(j)|

0 1 2 3 4 5 6 7 8 9 100

1

2

H0 = 3

4

5

6

7

Whe

re is

the

peak

?

How high?

w = 0:0.01:10;

s = j*w;

H = 48./(s.^2 + 2*s + 16);

r

Hpk

Page 15: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Magnitude Response

• For what values of is there a peak?

• Where are the peaks?

• How high are the peaks?

|H(j)| = 0.1

0.2

0.3

0.7

n2n0

0

1

3

5

0.60.5

0.4

Page 16: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Where is Peak in Mag Response?Peak in |H(j)|2 happens when magnitude-squared of denom is minimized:

(n2 – 2)2 + (2n)2

=

⇒ 2 – n2 + 22n

2 = 0

⇒ = “resonant frequency”

Resonant peak exists only when < ≈0.707!

Value of peak? Evaluating at r yields .

Depends only on

d

d-------

2(n2 – 2)(–2) + 2(2n)2n = 0

r = n 1 22–

1/2

Hpk

H0

--------- 1

2 1 2–-------------------------=

Page 17: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Resonant Peak Pole Locations

RESONANT PEAK ONLY

= 0

= 0.707

= 1

IN SHADED REGION

Page 18: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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From Mag Response to n and

|H(j)|

00

Page 19: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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From Mag Response to n and

|H(j)|

0

H0

Hpk 1) Solve Hpk/H0 = for 1

2 1 2–-------------------------

H0

Hpk-------- = sin( sin–1( ))1

2---

Page 20: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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From Mag Response to n and

|H(j)|

r0

H0

Hpk 1) Solve Hpk/H0 = for 1

2 1 2–-------------------------

2) Solve r = n for n1 22–

H0

Hpk-------- = sin( sin–1( ))1

2---

Page 21: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Peak vs Damping Coeff

0 0.1 0.2 0.3 0.4 0.5 0.6 0.71

10

Hpk/H

0=

1

2

12

–----

--------

--------

-----

H0

Hpk-------- = sin( sin–1( ))1

2---

2

3

4

5

Page 22: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Relationship to Pole Locationspeak height Hpk/H0 depends only on = cos

Page 23: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Relationship to Pole Locationspeak height Hpk/H0 depends only on = cos

SAME Hpk/H0

Hpk/H0

Hpk/H0

Page 24: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Pop Quiz

0 100 200 300 4000

2

4

6

8

10

12

14

16

18

|H(j)|

⇒ H( s ) = where

H0 =

n =

=

H0n2

s2 2n s n2+ +

-----------------------------------------------

Page 25: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Time Domain Properties of

2nd Order Systems

Page 26: Reminder: •HW11 due Thursday Lecture: 2nd-order systems ...barry.ece.gatech.edu/3084/lectures/lec27.pdf · 0 Lecture 27: Tue Nov 17, 2020 Reminder: •HW11 due Thursday Lecture:

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Underdamped LPF Step ResponseCan’t measure n and directly, but can derive them from measurements of:

steady-state value (determines H0)

percentage overshoot (determines )

peak time

settling time (given , determines n)

0 t

y( t )

tpk

STEP RESPONSE

tsettle

1.02H0

0.98H0

H0

(1 + )H0


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