Warning: foreach() argument must be of type array|object, bool given in /var/www/html/web/app/themes/studypress-core-theme/template-parts/header/mobile-offcanvas.php on line 20

Show that moment of inertia of a disk of mass M and radius R is 12MR2. Divide the disk into narrow rings, each of radius r and width dr. The contribution I of by one of these rings is r2dm, where dm is amount of mass contained in that particular ring. The mass of any ring is the total mass times the fraction of the total area occupied by the area of the ring. The area of this ring is approximately 2πrdr. Use integral calculus to add up all the calculations.

Short Answer

Expert verified

It is proved that the moment of inertia of disk is 12MR2.

Step by step solution

01

Identification of given data

The mass of disk is M.

The radius of disk is R.

The radius of each ring is r.

The width of each ring is dr.

The mass of each ring is dm.

The moment of inertia of each ring is I=r2dm.

02

Conceptual Explanation

The moment of inertia of the disk is obtained by calculating mass of each ring then substitute in the formula for mass of each ring.

03

Determination of moment of inertia of disk

The density of disk is given as:

ρ=MπR2r

The volume of each ring is given as:

V=2πrdrrdV=2πr2dr

The mass of each ring is given as:

dm=ρdVdm=MπR2r2πr2drdm=2MR2rdr

The moment of inertia of disk is calculated as:

Id=0RIId=0Rr2dmId=0Rr22MR2rdrId=2MR20Rr3dr

Id=2MR2r440RId=2MR2R44Id=12MR2

Therefore, the moment of inertia of disk is 12MR2.

Unlock Step-by-Step Solutions & Ace Your Exams!

  • Full Textbook Solutions

    Get detailed explanations and key concepts

  • Unlimited Al creation

    Al flashcards, explanations, exams and more...

  • Ads-free access

    To over 500 millions flashcards

  • Money-back guarantee

    We refund you if you fail your exam.

Over 30 million students worldwide already upgrade their learning with Vaia!

One App. One Place for Learning.

All the tools & learning materials you need for study success - in one app.

Get started for free

Most popular questions from this chapter

Consider the acceleration of a car on dry pavement, if there is no slipping. The axle moves at speed v, and the outside of the tire moves at a speed relative to the axle. The instantaneous velocity of the bottom of the tire is zero. How much work is done by the force exerted on the tire by the road? What is the source of the energy that increases the car’s translational kinetic energy?

A rod of length Land negligible mass is attached to a uniform disk of mass Mand radius R (Figure 9.64). A string is wrapped around the disk, and you pull on the string with a constant force F . Two small balls each of mass mslide along the rod with negligible friction. The apparatus starts from rest, and when the center of the disk has moved a distance d, a length of string shas come off the disk, and the balls have collided with the ends of the rod and stuck there. The apparatus slides on a nearly frictionless table. Here is a view from above:

(a) At this instant, what is the speed vof the center of the disk? (b) At this instant the angular speed of the disk isω . How much internal energy change has there been?

By calculating numerical quantities for a multiparticle system. One can get a concrete sense of the meaning of the relationships psys=MtotvCMand Ktot=Ktrans+Krel. Consider an object consisting of two balls connected by a spring, whose stiffness is 400 N/m. The object has been thrown through the air and is rotating and vibrating as it moves. At a particular instant, the spring is stretched 0.3m, and the two balls at the ends of the spring have the following masses and velocities: 1:5kg.(8,14,0)m/s2:3kg(-5,9,0)m/s

(a)For this system, calculate psys. (b) Calculate vCM(c) Calculate Ktot3. (d) Calculate Ktrans. (e) Calculate Krel. (f) Here is a way to check your result for Krel. The velocity of a particle relative to the center of mass is calculated by subtracting vCMfrom the particle’s velocity. To take a simple example, if you’re riding in a car that’s moving with vCM,x=20m/sand you throw a ball with vCM,x=35m/s, relative to the car, a bystander on the ground sees the ball moving with vx=55m/sSo v=vCM=vreland therefore we have=vrelv=vCMfor each mass and calculate the correspondingKrel. Compare with the result you obtained in part (e).

A runner whose mass is 50kg accelerates from a stop to a speed of 10m/s in 3s. (A good sprinter can run 100m in about 10s, with an average speed of 10m/s.) (a) What is the average horizontal component of the force that the ground exerts on the runner’s shoes? (b) How much displacement is there of the force that acts on the sole of the runner’s shoes, assuming that there is no slipping? Therefore, how much work is done on the extended system (the runner) by the force you calculated in the previous exercise? How much work is done on the point particle system by this force? (c) The kinetic energy of the runner increases—what kind of energy decreases? By how much?

A solid uniform-density sphere is tied to a rope and moves in a circle with speed v. The distance from the center of the circle to the center of the sphere is M, the mass of the sphere is, and the radius of the sphere is R. (a) What is the angular speedω? (b) What is the rotational kinetic energy of the sphere? (c) What is the total kinetic energy of the sphere?

See all solutions

Recommended explanations on Physics Textbooks

View all explanations

What do you think about this solution?

We value your feedback to improve our textbook solutions.

Study anywhere. Anytime. Across all devices.

Sign-up for free