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10/22/2014PHY 711 Fall Lecture 243
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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
PHY 711 Fall 2014 -- Lecture 24 210/22/2014
PHY 711 Fall 2014 -- Lecture 24 310/22/2014
PHY 711 Fall 2014 -- Lecture 24 410/22/2014
PHY 711 Fall 2014 -- Lecture 24 510/22/2014
The physics of rigid body motion; body fixed frame vs inertial frame:
PHY 711 Fall 2014 -- Lecture 24 610/22/2014
Comparison of analysis in “inertial frame” versus “non-inertial frame”
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system coordinate moving a ˆby Denote
system coordinate fixed a ˆby Denote
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03
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V
V
V
PHY 711 Fall 2014 -- Lecture 24 710/22/2014
Properties of the frame motion (rotation):
dQ
dQye
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eded
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PHY 711 Fall 2014 -- Lecture 24 810/22/2014
VωVV
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Effects on acceleration:
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bodybodyinertial
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2
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PHY 711 Fall 2014 -- Lecture 24 910/22/2014
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:body rigid ofenergy Kinetic
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PHY 711 Fall 2014 -- Lecture 24 1010/22/2014
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PHY 711 Fall 2014 -- Lecture 24 1110/22/2014
x
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: tensorinertia ofMoment
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Example:
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
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: tensorinertia ofMoment
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PHY 711 Fall 2014 -- Lecture 24 1310/22/2014
Changing origin of rotation ''''
2
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:mass ofcenter theDefine
'
M
m
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mp
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2' 2CMjijCMiijCMjiijijij rRRrMRRRMII Rr
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ya
c
b
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y’
x’
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PHY 711 Fall 2014 -- Lecture 24 1410/22/2014
2' 2CMjijCMiijCMjiijijij rRRrMRRRMII Rr
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cba
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and ˆˆˆ that Suppose
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PHY 711 Fall 2014 -- Lecture 24 1510/22/2014
000000
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c
b
z’
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PHY 711 Fall 2014 -- Lecture 24 1610/22/2014
Descriptions of rotation about a given origin
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: tensorinertia ofmoment esdiagonaliz that system coordinate fixed)(body For
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PHY 711 Fall 2014 -- Lecture 24 1710/22/2014
Descriptions of rotation about a given origin -- continued
3122123113
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: tensorinertia ofmoment esdiagonaliz that system coordinate fixed)(body For
momentumangular of change of rate Time
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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~
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: tensorinertia ofmoment esdiagonaliz that system coordinate fixed)(body For
momentumangular of change of rate Time
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iii
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PHY 711 Fall 2014 -- Lecture 24 1910/22/2014
Descriptions of rotation about a given origin -- continued
0ˆ~~ˆ~~
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:equationsEuler thesolvecan we0For frame. fixedbody in thedirectly solve todifficult very is
equation torque that theNote
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PHY 711 Fall 2014 -- Lecture 24 2010/22/2014
0~~~
0~~~0~~~
:frame fixedbody in rotation for equationsEuler
122133
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III
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1
133
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(constant)~ 0~0~~~0~~~
: -- topsymmetricfor Solution
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12
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PHY 711 Fall 2014 -- Lecture 24 2110/22/2014
Solution of Euler equations for a symmetric top -- continued
)sin()(~ )cos()(~ :Solution
~ where
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1
1
133
1221
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PHY 711 Fall 2014 -- Lecture 24 2210/22/2014
0~~~
0~~~0~~~
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2
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~ :Define 0~ :Suppose
0~~~0~~~0~~~
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