A disk of mass 3 kgand radius0.15 mhangs in the xy plane from a horizontal low-friction axle. The axle is 0.09 m from the center of the disk. What is the frequencyof small-angle oscillations of the disk? What is the period?

Short Answer

Expert verified

The frequency of small angle oscillation of the disk is 1.07Hz.

Step by step solution

01

Define the frequency of Oscillations.

The frequency of the oscillation is the number of oscillations in one second. If the particle completes one oscillation in T seconds, then the number of oscillations in one second or frequency is given as,

f=1T

The frequency of oscillation is measured in Hertz.

02

About the period of oscillations:

The period of the oscillations of a disk in a vertical plane through the point S is,

T=2πIsMgh ….. (1)

Here, Is is moment of inertia of the disk relative to Mis mass of the disk, his distance from the centre of mass of disk to the suspension point S and g is acceleration due to gravity.

03

Figure shows that the oscillations of a disk in a vertical plane: 

The diagram shows the oscillations of a disk in a vertical plane supported by a horizontal axis through a point S.

04

Find the frequency of the disk: 

The moment of inertia of the disk relative to pointOis,

IO=12MR2

Here, M is mass of the disk and is radius of the disk.

Thus, the moment of inertia of the disk relative to is,

Is=IO+Mh2=12MR2+Mh2

Substitute for into equation (1).

T=2π12MR2+Mh2Mgh=2πR2+2h22gh

Substitute 0.15 m for R, 0.09 forh , and 9.8m/s2 for g in the above equation.

T=2×3.140.15m2+20.09m2(9.8m/s2)0.09m

T=6.280.0225+0.0162m21.764m2/s2=6.280.148s=0.93s

Therefore, the period of the oscillations of a disk is 0.93s.

The frequency of small angle oscillation of the disk is,

f=1T

Substitute 0.93sfor T

f=10.93s=1.07Hz

Hence, the frequency of small angle oscillation of the disk is 1.07Hz.

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Most popular questions from this chapter

A device consists of eight balls, each of massattached to the ends of low-mass spokes of length L so the radius of rotation of ball is L/2. The device is mounted in the vertical plane, as shown in Figure 11.73. The axle is help up by supports that are not shown, and the wheel is free to rotate on the nearly frictionless axle. A lump of clay with massm falls and sticks to one of the balls at the location shown, when the spoke attached to that ball is 45°to the horizontal. Just before the impact the clay has a speed v, and the wheel is rotating counter clock wise with angular speedω .

(a.) Which of the following statements are true about the device and the clay, for angular momentum relative to the axle of the device? (1) the angular momentum of the device + clay just after the collision is equal to the angular momentum of the device +clay just before the collision. (2) The angular momentum of the falling clay is zero because the clay is moving in a straight line. (3) Just before the collision, the angular momentum of the wheel is 0. (4) The angular momentum of the device is the sum of the angular momenta of all eight balls. (5) The angular momentum of the device is the same before and after the collision. (b) Just before the impact, what is the (vector) angular momentum of the combined system of device plus clay about the center C? (As usual, xis to the right, yis up, and zis out of the screen, toward you) (c) Just after the impact, what is the angular momentum of the combined system of device plus clay about the center C? (d) Just after the impact, what is the (vector) angular velocity of the device? (e) Qualitatively. What happens to the total linear momentum is changed system? Why? (1) some of the linear momentum is changed into energy. (2) some of the linear momentum is changed into angular momentum. (3) There is no change because linear momentum is always conserved. (4) The downward linear momentum decreases because the axle exerts an upwards force. (f) qualitatively, what happens to the total kinetic energy of the combined system? Why? (1) some of the kinetic energy is changed into linear momentum. (2) some of the kinetic energy is changed into angular momentum. (3) The total kinetic energy decreases because there is an increase of internal energy in this inelastic collision. (4) There is no change because kinetic energy is always conserved.

At a particular instant the location of an object relative to location \(A\) is given by the vector \({\overrightarrow r _A} = \left\langle {6,6,0} \right\rangle {\rm{m}}\). At this instant the momentum of the object is \(\overrightarrow p = \left\langle { - 11,13,0} \right\rangle {\rm{kg}} \cdot {\rm{m}}/{\rm{s}}.\) What is the angular momentum of the object about location \(A\)?

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Give an example of a situation in which an object is traveling a straight line, yet has non-zero angular momentum.

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