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Physics 170 - Lecture 27 Angular

For a particle of m moving in a of radius r:

More generally: L = r x p Angular Momentum

For more general , Sign of Angular Momentum

L>0 L>0

The angular momentum L is taken to be positive if the angular is increasing with , i.e., if the motion associated with L is a counterclockwise . Rotation as a Vector

We can treat rotation and other angular motion quantities as vectors by using the right-hand rule: if the fingers of your right hand follow the rotation direction, then your thumb points along the rotation axis in the vector direction of the angular ω.

An alternative definition is that if a right-hand threaded screw is rotated, then ω points in the direction in which the screw advances. The Vector Nature of Rotational Motion

Similar application of the right-hand rule gives the vector direction of the τ. The Vector Nature of Rotational Motion

The vector directions of the vector ω and the angular momentum vector L are along the axis of rotation. Applying the right-hand rule gives the direction. Angular Momentum and Angular Velocity as Vectors Example: Angular Momentum About the Origin Find the angular momentum about the origin for the following situations:

(a) A car of mass 1200 kg moves in a counterclockwise circle in the xy plane of radius 20 m with a speed of 15 m/s; (b) A uniform disk in the xy plane of radius 20 m and mass 1200 kg rotates at 0.75 rad/s along its axis, which is the z axis. Example: Angular Momentum

(a) What is the angular momentum of a 0.13 kg Frisbee, considered to be a uniform disk of radius 7.5 cm, spinning with ω = 11.5 rad/s?

(b) What is the angular momentum of a 95 kg person running with a speed of 5.1 m/s around a circular track of radius 25 m? Example: The Spin Angular Momentum of the

What is the angular momentum of the Earth as it rotates on its axis? (Assume a uniform sphere.) Example: The Orbital Angular Momentum of the Earth

What is the angular momentum of the Earth as it the ? Changing Angular Momentum

Looking at the at which angular momentum changes,

Therefore, if τ = 0, then L is constant with time. If the net external torque on a system is zero, the angular momentum is conserved. Example: A Windmill

In a light , a windmill experiences a constant torque of 255 N m.

If the windmill is initially at rest, what is its angular momentum after 2.00 s?

Notice that you do not need to know the of of the windmill to do this calculation. Example: Jumping On

Running with a speed of 4.10 m/s, a 21.2 kg child heads toward the rim of a merry-go-round of radius 2.00 m, as shown.

What is the child’s angular momentum L with respect to the center of the merry-go-round?

(L = r x p) Conservation of Angular Momentum If the net external torque on a system is zero, the angular momentum is conserved.

The most interesting consequences occur in systems that are able to change shape:

3.74 rad/s

5.33 kg m2 1.60 kg m2 Example: A Stellar Performance

8 A star of radius Ri = 2.3 x 10 m rotates initially with -6 an angular speed of ωi = 2.4 x 10 rad/s.

If the star collapses to a neutron star of radius Rf =

20.0 km, what will be its final angular speed ωf ?