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10/22/2014 PHY 711 Fall 2014 -- Lecture 24 1 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational motion (Chapter 5) 1.Rigid body motion 2.Moment of inertia tensor

10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

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Page 1: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 110/22/2014

PHY 711 Classical Mechanics and Mathematical Methods

10-10:50 AM MWF Olin 103

Plan for Lecture 24:Rotational motion (Chapter 5)

1. Rigid body motion2. Moment of inertia tensor

Page 2: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 210/22/2014

Page 3: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 310/22/2014

Page 4: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 410/22/2014

Page 5: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 510/22/2014

The physics of rigid body motion; body fixed frame vs inertial frame:

Page 6: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 610/22/2014

Comparison of analysis in “inertial frame” versus “non-inertial frame”

dtedV

dtd

dtd

edt

dVdtd

dtedVe

dtdVe

dtdV

dtd

eVeV

e

e

i

ii

bodyinertial

ii

i

body

i

iii

i

ii

i

i

inertial

ii

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i

i

i

ˆ

ˆ :Define

ˆˆˆ

ˆˆ

system coordinate moving a ˆby Denote

system coordinate fixed a ˆby Denote

3

1

3

1

3

1

3

1

03

1

0

3

1

03

1

0

0

VV

V

V

V

Page 7: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 710/22/2014

Properties of the frame motion (rotation):

dQ

dQye

ze

yed ˆ

zed ˆ

eωe

eeee

ˆˆ

ˆˆˆˆ

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Q

dtd

dtd

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dd

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eded

yz

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z

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z

y

z

y

ee

ee

dddd

eded

ˆˆ

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cossinsincos

ˆˆ

Page 8: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 810/22/2014

VωVV

VV

bodyinertial

i

ii

bodyinertial

dtd

dtd

dtedV

dtd

dtd ˆ3

1

Effects on acceleration:

VωωVωVωVV

VωVωV

dtd

dtd

dtd

dtd

dtd

dtd

dtd

dtd

bodybodyinertial

bodybodyinertial

22

2

2

2

Page 9: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 910/22/2014

rωrr

bodyinertial dtd

dtd

:body rigid ofenergy Kinetic

r

w

2

22

21

21

21

21

ωrrrωω

rωrω

rωr

pppp

p

pp

pp

ppp

ppp

inertial

m

m

mvmT

dtd

Page 10: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1010/22/2014

ωIω

ωrrrωω

21 2

pppp

pmT

notation) (dyad

: tensorinertia ofMoment 2

ppppp rm rr1I

:notationMatrix

2

ppjpipijpij

zzzyzx

yzyyyx

xzxyxx

rrrmI

IIIIIIIII

I�

Page 11: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1110/22/2014

x

z

ya

c

b

: tensorinertia ofMoment

2231

41

41

4122

31

41

41

4122

31

babcac

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MI�

Example:

Page 12: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1210/22/2014

Properties of moment of inertia tensor: Symmetric matrix real eigenvalues I1,I2,I3

orthogonal eigenvectors3,2,1 ˆˆ iI iii eeI

: tensorinertia ofMoment

2231

41

41

4122

31

41

41

4122

31

babcac

bccaabacabcb

MI�

1211

1211

61

:For

23

22

21 Ma IMa IMaI

cba

Page 13: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1310/22/2014

Changing origin of rotation ''''

2

2

ppjpipijpij

ppjpipijpij

rrrmI

rrrmI

:mass ofcenter theDefine

'

M

m

m

mp

pp

pp

ppp

CM

pp

rrr

Rrr

2' 2CMjijCMiijCMjiijijij rRRrMRRRMII Rr

x

z

ya

c

b

z’

y’

x’

Rrp r’p

Page 14: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1410/22/2014

2' 2CMjijCMiijCMjiijijij rRRrMRRRMII Rr

RrzyxR

cba

CM

222

and ˆˆˆ that Suppose

' 2jiijijij RRRMII

'

2241

41

41

4122

41

41

41

4122

41

2231

41

41

4122

31

41

41

4122

31

babcacbccaabacabcb

M

babcacbccaabacabcb

MI�

x

z

ya

c

b

z’

y’

x’

Rrp r’p

Page 15: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1510/22/2014

000000

'22

121

22121

22121

baca

cbMI

�x

z

ya

c

b

z’

y’

x’

Rrp r’p

Page 16: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1610/22/2014

Descriptions of rotation about a given origin

iii

iii

jij

iij

IT

iI

IT

2

332211

~21

ˆ~ˆ~ˆ~3,2,1 ˆˆ

: tensorinertia ofmoment esdiagonaliz that system coordinate fixed)(body For

21

system coordinate generalFor

w

www

ww

eeeωeeI

Page 17: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1710/22/2014

Descriptions of rotation about a given origin -- continued

3122123113

12332333222111

333222111

332211

ˆ~~ˆ~~

ˆ~~ˆ~ˆ~ˆ~

ˆ~ˆ~ˆ~ˆ~ˆ~ˆ~ ˆˆ

: tensorinertia ofmoment esdiagonaliz that system coordinate fixed)(body For

momentumangular of change of rate Time

ee

eeeeLeeeL

eeeωeeI

LωLL

IIII

IIIIIdtd

IIII

dtd

dtd

iii

body

wwww

wwwww

wwwwww

Page 18: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1810/22/2014

Descriptions of rotation about a given origin -- continued

3122123113

12332333222111

333222111

332211

ˆ~~ˆ~~

ˆ~~ˆ~ˆ~ˆ~

ˆ~ˆ~ˆ~ˆ~ˆ~ˆ~ ˆˆ

: tensorinertia ofmoment esdiagonaliz that system coordinate fixed)(body For

momentumangular of change of rate Time

ee

eeeeLeeeL

eeeωeeI

LωLL

IIII

IIIIIdtd

IIII

dtd

dtd

iii

body

wwww

wwwww

wwwwww

Page 19: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 1910/22/2014

Descriptions of rotation about a given origin -- continued

0ˆ~~ˆ~~

ˆ~~ˆ~ˆ~ˆ~

:equationsEuler thesolvecan we0For frame. fixedbody in thedirectly solve todifficult very is

equation torque that theNote

3122123113

12332333222111

ee

eeeeLτ

τLωLL

IIII

IIIIIdtd

dtd

dtd

body

wwww

wwwww

Page 20: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 2010/22/2014

0~~~

0~~~0~~~

:frame fixedbody in rotation for equationsEuler

122133

311322

233211

III

III

III

www

www

www

1

133

333

311321

133211

12

~ :Define

(constant)~ 0~0~~~0~~~

: -- topsymmetricfor Solution

IIIΩ

I

III

III

II

w

ww

www

www

12

21

~~

~~

ww

ww

Page 21: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 2110/22/2014

Solution of Euler equations for a symmetric top -- continued

)sin()(~ )cos()(~ :Solution

~ where

~~ ~~

2

1

1

133

1221

ww

w

wwww

tAttAt

IIIΩ

233

21

2 ~21

21~

21 ww IAIIT

iii

Page 22: 10/22/2014PHY 711 Fall 2014 -- Lecture 241 PHY 711 Classical Mechanics and Mathematical Methods 10-10:50 AM MWF Olin 103 Plan for Lecture 24: Rotational

PHY 711 Fall 2014 -- Lecture 24 2210/22/2014

0~~~

0~~~0~~~

:frame fixedbody in rotation for equationsEuler

122133

311322

233211

III

III

III

www

www

www

2

1332

1

23313

122133

311322

233211

123

~ :Define

~ :Define 0~ :Suppose

0~~~0~~~0~~~

: -- topasymmetricfor Solution

IIIΩ

IIIΩ

III

III

III

III

w

ww

www

www

www