mechanical vibration by palm chapter 4: harmonic response with a single degree of freedom...

20
Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based on a lecture from Brown university (Division of engineering)

Upload: javon-lone

Post on 31-Mar-2015

223 views

Category:

Documents


8 download

TRANSCRIPT

Page 1: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Mechanical Vibration by Palm

CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF

FREEDOM

Instructor: Dr Simin Nasseri, SPSU

© Copyright, 2010 1Based on a lecture from Brown university (Division of engineering)

Page 2: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

External Forcing Base Excitation

Types of Forcing:

Rotor Excitation

All of these situations are of practical interest. Some subtle but important distinctions to consider, so we will look at each.

But the strategy is simple: derive Equation of Motion and put into the “Standard Form”

Page 3: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

3

Base Excitation (Seismic motion)

Page 4: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

4

Base Excitation (Seismic motion)

Page 5: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Base Excitation – the Earthquake Problem

Here, base supporting object is subjected to motion.

How does the object respond?

Forces in the spring, dashpot are proportional to the motion RELATIVE to the base

Draw F.B.D. and get equation of motion….

)sin()( tYty

)(tx

2

2( ) ( )vertical

dx dy d xF k x y c m

dt dt dt

2

2

d x dx dym c kx ky c

dt dt dt

2

2sin( ) cos( )

d x dxm c kx kY t c Y t

dt dt

22 2

2( ) ( ) sin( )

d x c dx k kY c Yx t

dt m dt m m m

Page 6: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

22 2 2 2

22 ( ) (2 ) sin( )n n n n

d x dxx Y Y t

dt dt

22 2 2

22 1 (2 / ) sin( )n n n n

d x dxx Y t

dt dt

Now in the “standard form” but with a new “driving force” 22 )/2(1 nno YmF

2222

21

1

nn

n

o

m

FX

222

2

21

)/2(1

nn

n

Y

X

(Displacement Amplitude of body)/(Displacement Amplitude of Base)

22 2

2( ) ( ) sin( )

d x c dx k kY c Yx t

dt m dt m m m

Page 7: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Harmonic Base Excitation

Displacement transmission ratio: 222

2

21

)2(1

rr

r

Y

X

0 0.5 1 1.5 2 2.5 30

1

2

3

4

5

6

Y

X

rn /

1.0

2.0

3.0

0.11.0

Page 8: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Base Isolation Concept:

“soft” spring

Given an expected frequency of a driving force,

Design spring/dashpot coupling to minimize response

Clearly want to get in the regime 1/ n n

“soft” springs (small k)

Non-isolated Isolated

Page 9: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

04_03_02

9

Page 10: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Design of Car Suspension for Wavy Roads:

Car weighing 3000 lbs drives over a road with sinusoidal profile shown

k c

m

s

16”

33 ft

Design the suspension so that:

1. The vibration amplitude of the car is < 14” at all speedsand2. The vibration amplitude of the car is < 4” at 55 mph

Select springs (k) and shocks (c) to satisfy requirements of maximum car vibration amplitude when driving on a wavy roadx(t)

Page 11: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

What is the “base excitation” here?

Equation of road profile?16”

33 ft

As car drives along at constant speed, it is as if the road is vibrating up and down underneath the car

OK, but how do we represent that? ftLftY 33 ; 667.0"8

)2

sin( L

VtYy

L

V 2Driving frequency of base is

Design requirements are now:

(Vibration amplitude < 14” at all speeds)

1. at all frequencies75.18

14

Y

X

5.08

4

Y

X2. at frequency s

rad

ft

sftx36.15

33

)3600/528055(2

t

VLYt

TYtYy

/

2sin

2sin)sin(

Page 12: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

0 0.5 1 1.5 2 2.5 30

0.5

1

1.5

2

2.5

3

3.5

4

Let’s do this graphically, using our magnification plot:

Y

X

50.0,.....15.0,10.0,05.0

1.75 35.0~

0.5

35.0

n /2/55 nMPh

2/55 nMPh will satisfy criterion #2 for =0.35

35.0 will satisfy criterion #1

Page 13: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

2/55 nMPh

35.0

nMPh 2/55

sradn /2

36.15 sradn /68.7

Spring k required: ftlbsft

lbsmk n /495,5)

/2.32

3000()/68.7(

222

Damping c required: ftslbssft

lbmc n /500)/68.7)(

/2.32

3000)(35.0(22

2

Page 14: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

14

Summary:

Page 15: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Harmonic Base Excitation – Motion Relative to Base

Sometimes the motion relative to the base is of interest 2

2( ) ( )

dx dy d xk x y c m

dt dt dt

Introducing the relative displacement z = x – y, the equation of motion becomes:2 2

2 2( )

dz d z d ykz c m

dt dt dt

2 2

2 2

d z dz d ym c kz m

dt dt dt Or:

22 2

22 sin( )n n

d z dzz Y t

dt dt

mFo /

2222

21

1

nn

n

o

m

FX

222

2

21nn

n

Y

Z

Page 16: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

0 0.5 1 1.5 2 2.5 30

1

2

3

4

5

6

7

8

9

10

MY

Zn

nn

n 2

222

2

21

Y

Z

nLow frequencies: body

moves with base – no relative motion

High frequencies: base is moving but body is not, so relative motion = 1

Page 17: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

17

Page 18: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Goal: Detect “Low Frequency Earthquake” tremors in the 1-5 Hz frequency range along the San Andreas fault.

Constraints: Background vibrations over a wide range of higher frequencies occur with typical amplitudes of 0.1mm, so tremor amplitudes comparable to or smaller than this cannot be detected.

Design a mass/spring/dashpot system (choose m, k, c) to:(i)reliably detect tremors at a frequency of 3 Hz and having earth motion amplitudes of 0.01mm or larger,(ii) ensure that the maximum amplitude will not exceed 30 mm for earth motion amplitudes of 1.0 mm.

Design of a Seismograph:

Note: device measures motions relative to its base

FYI

Page 19: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

Example: The motion of the outer cart is varying sinusoidally

as shown.

For what range of is the amplitude of the motion of the mass m, relative to the cart less than 2b?

2

22 2

2 1

n

n n

Z

Y

2

2

1

n

n

Z

Y

when no damping

2

22

1

n

n

Z

Y

Two solutions:

(When )n And: (When )n

2

2

1

n

n

Z

Y

Page 20: Mechanical Vibration by Palm CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM Instructor: Dr Simin Nasseri, SPSU © Copyright, 2010 1 Based

We want 2

2Z b

Y b

2

2 2

1

n

n

2

3n

2

2 2

1

n

n

2n

n for

n for 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2 2.2

-2.5

-2

-1.5

-1

-0.5

0

0.5

1

1.5

2

2.5

(0.817)

(1.414)