A wheel with \(c=\frac{4}{9}\), a mass of \(40.0 \mathrm{~kg}\), and a rim radius of \(30.0 \mathrm{~cm}\) is mounted vertically on a horizontal axis. A 2.00 -kg mass is suspended from the wheel by a rope wound around the rim. Find the angular acceleration of the wheel when the mass is released.

Short Answer

Expert verified
#tag_title#Answer#tag_content# When the mass is released, the angular acceleration of the wheel is given by the formula: \(α = \frac{\tau}{I} = \frac{rF}{\frac{1}{2}MR^2}\). First, we calculate the force exerted by the suspended mass: \(F = mg = (2.00 \mathrm{~kg})(9.81 \mathrm{~m/s^2}) = 19.62 \mathrm{~N}\). Next, we calculate the moment of inertia of the wheel: \(I = \frac{1}{2}(40.0 \mathrm{~kg})(0.3 \mathrm{~m})^2 = 1.8 \mathrm{~kg \cdot m^2}\). Now, we substitute the values of torque and moment of inertia into the formula for angular acceleration: \(α = \frac{(0.3 \mathrm{~m})(19.62 \mathrm{~N})}{1.8 \mathrm{~kg \cdot m^2}} = 3.27 \mathrm{~rad/s^2}\). Therefore, the angular acceleration of the wheel when the mass is released is \(3.27 \mathrm{~rad/s^2}\).

Step by step solution

01

Identify the forces acting on the system

There are two forces acting on the system: the gravitational force acting on the suspended mass and the tension in the rope. The gravitational force acting on the mass causes it to accelerate downward and exerts a torque on the wheel, causing it to rotate. The tension in the rope opposes the gravitational force and also exerts a torque on the wheel.
02

Determine the moment of inertia of the wheel

To calculate the moment of inertia for the wheel, we can use the formula for a solid cylinder, \(I = \frac{1}{2}MR^2\) where \(M\) is the mass of the wheel, and \(R\) is the rim radius. The moment of inertia of the wheel is: \(I = \frac{1}{2}(40.0 \mathrm{~kg})(0.3 \mathrm{~m})^2\)
03

Calculate the torque acting on the wheel due to the suspended mass

The torque acting on the wheel due to the suspended mass can be estimated using the formula: \(\tau = rF\), where \(r\) is the radius of the rim, and \(F\) is the force exerted by the suspended mass (the gravitational force acting on the mass). The force exerted by the suspended mass is: \(F = mg\), where \(m = 2.00 \mathrm{~kg}\) (the mass of the suspended weight), and \(g = 9.81 \mathrm{~m/s^2}\) (acceleration due to gravity).
04

Use Newton's second law for rotation to find the angular acceleration

Newton's second law for rotation states that the angular acceleration (α) is equal to the torque (τ) divided by the moment of inertia (I): \(α = \frac{\tau}{I}\). Substituting the expressions for torque and moment of inertia, we find the angular acceleration when the mass is released.

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

A solid ball and a hollow ball, each with a mass of \(1.00 \mathrm{~kg}\) and radius of \(0.100 \mathrm{~m}\), start from rest and roll down a ramp of length \(3.00 \mathrm{~m}\) at an incline of \(35.0^{\circ} .\) An ice cube of the same mass slides without friction down the same ramp. a) Which ball will reach the bottom first? Explain! b) Does the ice cube travel faster or slower than the solid ball at the base of the incline? Explain your reasoning. c) What is the speed of the solid ball at the bottom of the incline?

In a tire-throwing competition, a man holding a \(23.5-\mathrm{kg}\) car tire quickly swings the tire through three full turns and releases it, much like a discus thrower. The tire starts from rest and is then accelerated in a circular path. The orbital radius \(r\) for the tire's center of mass is \(1.10 \mathrm{~m},\) and the path is horizontal to the ground. The figure shows a top view of the tire's circular path, and the dot at the center marks the rotation axis. The man applies a constant torque of \(20.0 \mathrm{~N} \mathrm{~m}\) to accelerate the tire at a constant angular acceleration. Assume that all of the tire's mass is at a radius \(R=0.35 \mathrm{~m}\) from its center. a) What is the time, \(t_{\text {throw }}\) required for the tire to complete three full revolutions? b) What is the final linear speed of the tire's center of mass (after three full revolutions)? c) If, instead of assuming that all of the mass of the tire is at a distance \(0.35 \mathrm{~m}\) from its center, you treat the tire as a hollow disk of inner radius \(0.30 \mathrm{~m}\) and outer radius \(0.40 \mathrm{~m}\), how does this change your answers to parts (a) and (b)?

A student of mass \(52 \mathrm{~kg}\) wants to measure the mass of a playground merry-go-round, which consists of a solid metal disk of radius \(R=1.5 \mathrm{~m}\) that is mounted in a horizontal position on a low-friction axle. She tries an experiment: She runs with speed \(v=6.8 \mathrm{~m} / \mathrm{s}\) toward the outer rim of the merry-go-round and jumps on to the outer rim, as shown in the figure. The merry-go-round is initially at rest before the student jumps on and rotates at \(1.3 \mathrm{rad} / \mathrm{s}\) immediately after she jumps on. You may assume that the student's mass is concentrated at a point. a) What is the mass of the merry-go-round? b) If it takes 35 s for the merry-go-round to come to a stop after the student has jumped on, what is the average torque due to friction in the axle? c) How many times does the merry-go-round rotate before it stops, assuming that the torque due to friction is constant?

A cylinder is rolling without slipping down a plane, which is inclined by an angle \(\theta\) relative to the horizontal. What is the work done by the friction force while the cylinder travels a distance \(s\) along the plane \(\left(\mu_{s}\right.\) is the coefficient of static friction between the plane and the cylinder)? a) \(+\mu_{s} m g s \sin \theta\) b) \(-\mu_{s} m g s \sin \theta\) c) \(+m g s \sin \theta\) d) \(-m g s \sin \theta\) e) No work done.

A light rope passes over a light, frictionless pulley. One end is fastened to a bunch of bananas of mass \(M,\) and \(a\) monkey of the same mass clings to the other end. The monkey climbs the rope in an attempt to reach the bananas. The radius of the pulley is \(R\). a) Treating the monkey, bananas, rope, and pulley as a system, evaluate the net torque about the pulley axis. b) Using the result of part (a) determine the total angular momentum about the pulley axis as a function of time

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