Handout 18 Inertia tensor n n Inertia tensor

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Handout #18 Inertia tensor n n Inertia tensor for a continuous body Kinetic energy

Handout #18 Inertia tensor n n Inertia tensor for a continuous body Kinetic energy from inertia tensor. Tops and Free bodies using Euler equations n n n Precession Lamina theorem Free-body wobble 1 : 02

Inertia Tensor For continuous body 2

Inertia Tensor For continuous body 2

Lamina Theorem 3 : 60

Lamina Theorem 3 : 60

L 18 -1 Angular Momentum and Kinetic Energy 1) A square plate of side

L 18 -1 Angular Momentum and Kinetic Energy 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? 4) L 4 : 02

Angular Momentum and Kinetic Energy We derived the moment of inertia tensor from the

Angular Momentum and Kinetic Energy 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) 5 : 02

L 18 -2 Angular Momentum and Kinetic Energy 1) A complex arbitrary system is

L 18 -2 Angular Momentum and Kinetic Energy 1) A complex arbitrary system is subject to multi-axis rotation. 2) The inertia tensor is 3) A 3 -axis rotation is 4) applied 5) 6 : 02

Symmetrical top Euler equation 7 : 02

Symmetrical top Euler equation 7 : 02

Precession Ignore in limit 8 : 02

Precession Ignore in limit 8 : 02

Euler’s equations for symmetrical bodies Note even for non-laminar symmetrical tops AND even for

Euler’s equations for symmetrical bodies Note even for non-laminar symmetrical tops AND even for 9 : 60

Euler’s equations for symmetrical bodies Precession frequency=rotation frequency for symmetrical lamina 10 : 60

Euler’s equations for symmetrical bodies Precession frequency=rotation frequency for symmetrical lamina 10 : 60

Euler’s equations for symmetrical bodies 11 : 60

Euler’s equations for symmetrical bodies 11 : 60

L 18 -3 – Chandler Wobble 1) The earth is an ovoid thinner at

L 18 -3 – Chandler Wobble 1) The earth is an ovoid thinner at the poles than the equator. 2) For a general ovoid, 3) For Earth, what are 12 : 60

Handout #18 windup 13 : 02

Handout #18 windup 13 : 02