1 Handout #18 Inertia tensor Inertia tensor for a continuous body Kinetic energy from inertia...
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Transcript of 1 Handout #18 Inertia tensor Inertia tensor for a continuous body Kinetic energy from inertia...
1
Handout #18
Inertia tensor Inertia tensor for a continuous
body Kinetic energy from inertia tensor.
Tops and Free bodies using Euler equations Precession Lamina theorem Free-body wobble
:02
2
Inertia Tensor For continuous body
2 2
2 2
2 2
( ) ( ) ( )
( ) ( ) .
... ( ) ( )
y z dxdydz xy dxdydz xz dxdydz
I yx dxdydz x z dxdydz etc
zy dxdydz x y dxdydz
3
Lamina Theorem
:60
zzIyyI
xxI
2 2 2 2
2 2
( ) ( )
( )
0
( 0)
xx yy
zz
zz xx yy xz yz
I I y z x z dxdydz
I x y dxdydz
I I I AND I I
for laminar objects z
yyIzzI
xxI
( 0)yy xx zzI I I for laminar objects y
4
L 18-1 Angular Momentum and Kinetic Energy
:02
1) A square plate of side L and mass M is rotated about a diagonal.
2) In the coordinate system with the origin at lower left corner of the square, the inertia tensor is?
3) What are the eigenvalues and eigenvectors for this square plate?
L
5
Angular Momentum and Kinetic Energy
:02
We derived the moment of inertia tensor from the fundamental definitions of L, by working out the double cross-product
Do the same for T (kinetic energy)
1 1( )
2 21
( ) ( )21
2
T mv v r mv
T r mv vector identity
T L
( )
( )
p mv m r
L r m r
1
2T
L I
T I
6
L 18-2 Angular Momentum and Kinetic Energy
:02
L 1) A complex arbitrary system is subject
to multi-axis rotation.
2) The inertia tensor is
3) A 3-axis rotation is
applied
6.6 2.6 0.44
-2.6 4.4 2.2
0.44 2.2 8.8
I
5.0
8.2
3.0
.
?
.
Calculate L
What is special about
Calculate T
1
2T
L I
T I
7
Symmetrical top
:02
3 3 3 1 2 1 2
1 2 3
3 33
( )
0
0 con
a d
s
n
t
Euler equation
8
Precession
:02
ˆsinCM
dLr F
dt
dLR mg
dt
Ignore in limit
2 22 2 2 23 3z zL L L L L
3p sin
L
L
3 3
sin1
sin sinCM CM
p
R mgd dL
dt L dt L
R mg
9
Euler’s equations for symmetrical bodies
:60
1 1 2 3 2 3
2 2 3 1 3 1
3 3 1 2 1 2
( )
( )
( )
zzIyyI
xxI
2
2
1
41
22
xx yy
zz xx yy
For Disk I I MR
I I I MR
1 2 3
2 3 1
3 1 2
( 2 )
(2 )
2 ( )
1 2 3
2 3 1
3 0
Note even for non-laminar symmetrical tops AND even for
3 0 1 2, 0
10
3 zL
p
Euler’s equations for symmetrical bodies
:60
1 2 3
2 3 1
3 0
21 3 1
22 3 2
2 23p
Precession frequency=rotation frequency for symmetrical lamina
11
Euler’s equations for symmetrical bodies
:60
3 z
L
p
3 1 3 1
3 zL
p
12
L18-3 – Chandler Wobble
:60
1) The earth is an ovoid thinner at the poles than the equator.
2) For a general ovoid,
3) For Earth, what are
2 21( )
5xxI M a b
, ?yy zz pI and I and
2b
2a
yyIzzI
xxI
1 1 1 3 2 3
1 2 3 1 3 1
3 3
223 1
1 3 121
( )
( )
0
( )
2 2 2a b a b b 6400
20
a km
km
13
Handout #18 windup
:02
1
2T
L I
T I
3 3
CMp
R mgfor top
minzz xx yyI I I for la a
2 21( )
5xxI M a b for ellipsoid