The Merry-Go-Round A horizontal platform in the shape of a circular disk rotates freely in a horizontal plane about a frictionless, vertical axle (see figure). The platform has a mass M- 100 kg and a radius R- 1.8 m. A student whose mass is m - 64 kg walks slowly from the rim of the disk toward its center. If the angular speed of the system is 2.1 rad/s when the student is at the rim, what is the angular speed when she reaches a point r- 0.40 m from the center? As the student walks toward the center of the rotating platform, the angular speed of the system increases because the angular momentum of the system remains constant. M R.

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The Merry-Go-Round
A horizontal platform in the shape of a circular disk rotates freely in a horizontal plane about a frictionless, vertical axle (see figure). The
platform has a mass M- 100 kg and a radius R= 1.8 m. A student whose mass is m - 64 kg walks slowly from the rim of the disk toward its
center. If the angular speed of the system is 2.1 rad/s when the student is at the rim, what is the angular speed when she reaches a point
r- 0.40 m from the center?
As the student walks toward the center of the
rotating platform, the angular speed of the
system increases because the angular
momentum of the system remains constant.
M
SOLUTION
Conceptualize The speed change here is similar to those of the spinning skater and the neutron star in preceding discussions. This problem is
different because part of the moment of inertia of the system changes (that of the ---Select---v) while part remains fixed (that of the
---Select---v).
Categorize Because the platform rotates on a frictionless axle, we identify the system of the student and the platform as --Select-- v
system in terms of angular momentum.
Analyze
(Use the following as necessary: M, m, R, r, w, and w, Do not substitute numerical values; use variables only.)
Let us denote the moment of inertia of the platform as I and that of the student as I. We model the student as a particle.
Find the initial moment of inertia I, of the system (student plus platform) about the axis of rotation:
Find the moment of inertia of the system when the student walks to the position r< R:
Write the law of conservation of angular momentum to the system:
Io, - Ipo,
Substitute the moments of inertia:
GMR? + mr² », = (
Solve for the final angular speed:
MR2 + mR2
MR2 + mr2
Substitute numerical values to find the final angular speed (in rad/s):
Transcribed Image Text:The Merry-Go-Round A horizontal platform in the shape of a circular disk rotates freely in a horizontal plane about a frictionless, vertical axle (see figure). The platform has a mass M- 100 kg and a radius R= 1.8 m. A student whose mass is m - 64 kg walks slowly from the rim of the disk toward its center. If the angular speed of the system is 2.1 rad/s when the student is at the rim, what is the angular speed when she reaches a point r- 0.40 m from the center? As the student walks toward the center of the rotating platform, the angular speed of the system increases because the angular momentum of the system remains constant. M SOLUTION Conceptualize The speed change here is similar to those of the spinning skater and the neutron star in preceding discussions. This problem is different because part of the moment of inertia of the system changes (that of the ---Select---v) while part remains fixed (that of the ---Select---v). Categorize Because the platform rotates on a frictionless axle, we identify the system of the student and the platform as --Select-- v system in terms of angular momentum. Analyze (Use the following as necessary: M, m, R, r, w, and w, Do not substitute numerical values; use variables only.) Let us denote the moment of inertia of the platform as I and that of the student as I. We model the student as a particle. Find the initial moment of inertia I, of the system (student plus platform) about the axis of rotation: Find the moment of inertia of the system when the student walks to the position r< R: Write the law of conservation of angular momentum to the system: Io, - Ipo, Substitute the moments of inertia: GMR? + mr² », = ( Solve for the final angular speed: MR2 + mR2 MR2 + mr2 Substitute numerical values to find the final angular speed (in rad/s):
rad/s
Finalize As expected, the angular speed ---Select--
center of the platform. Do this calculation to show that this maximum angular speed is 4.8 rad/s. Notice that the activity described in this
problem is dangerous as discussed with regard to the Coriolis force in a previous chapter.
v. The fastest that this system could spin would be when the student moves to the
EXERCISE
Suppose the student in the example had jumped on to the rim of the merry-go-round without transferring any angular momentum to the merry-
go-round.
Hint
(a) What was the angular speed (in rad/s) of the merry-go-round before the student jumped on? Recall that with the student standing at the
outer edge, the angular speed is 2.1 rad/s.
rad/s
(b) By how much did the kinetic energy of the system change (in J) when the student jumped on?
AK =
Transcribed Image Text:rad/s Finalize As expected, the angular speed ---Select-- center of the platform. Do this calculation to show that this maximum angular speed is 4.8 rad/s. Notice that the activity described in this problem is dangerous as discussed with regard to the Coriolis force in a previous chapter. v. The fastest that this system could spin would be when the student moves to the EXERCISE Suppose the student in the example had jumped on to the rim of the merry-go-round without transferring any angular momentum to the merry- go-round. Hint (a) What was the angular speed (in rad/s) of the merry-go-round before the student jumped on? Recall that with the student standing at the outer edge, the angular speed is 2.1 rad/s. rad/s (b) By how much did the kinetic energy of the system change (in J) when the student jumped on? AK =
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