/*! This file is auto-generated */ .wp-block-button__link{color:#fff;background-color:#32373c;border-radius:9999px;box-shadow:none;text-decoration:none;padding:calc(.667em + 2px) calc(1.333em + 2px);font-size:1.125em}.wp-block-file__button{background:#32373c;color:#fff;text-decoration:none} Problem 78 A wheel of radius \(0.250 \mathr... [FREE SOLUTION] | 91Ó°ÊÓ

91Ó°ÊÓ

A wheel of radius \(0.250 \mathrm{~m},\) moving initially at \(43.0 \mathrm{~m} / \mathrm{s},\) rolls to a stop in \(225 \mathrm{~m}\). Calculate the magnitudes of its (a) linear acceleration and (b) angular acceleration. (c) Its rotational inertia is \(0.155 \mathrm{~kg} \cdot \mathrm{m}^{2}\) about its central axis. Find the magnitude of the torque about the central axis due to friction on the wheel.

Short Answer

Expert verified
(a) Linear acceleration: 4.11 m/s², (b) Angular acceleration: 16.44 rad/s², (c) Torque: 2.5482 Nm.

Step by step solution

01

Determine the Linear Acceleration

To find the linear acceleration, use the formula for motion with constant acceleration: \[v^2 = u^2 + 2as\]where \(v = 0\) m/s (final velocity), \(u = 43.0\) m/s (initial velocity), and \(s = 225\) m (distance). Solving for \(a\):\[0 = (43.0)^2 + 2a(225)\]\[a = \frac{-(43.0)^2}{2 \times 225}\]\[a = -4.11 \mathrm{~m/s^2}\]Thus, the linear acceleration is \(4.11 \mathrm{~m/s^2}\).
02

Calculate the Angular Acceleration

The relationship between linear acceleration \(a\) and angular acceleration \(\alpha\) is given by:\[a = r\alpha\]where \(r = 0.250 \mathrm{~m}\) is the radius of the wheel. Solving for \(\alpha\):\[\alpha = \frac{a}{r} = \frac{4.11}{0.250}\]\[\alpha = 16.44 \mathrm{~rad/s^2}\]The angular acceleration is \(16.44 \mathrm{~rad/s^2}\).
03

Find the Torque Due to Friction

Torque \(\tau\) can be found using the relation from rotational dynamics:\[\tau = I \alpha\]where \(I = 0.155 \mathrm{~kg \cdot m^2}\) is the rotational inertia and \(\alpha = 16.44\) rad/s². Substituting the values:\[\tau = 0.155 \times 16.44\]\[\tau = 2.5482 \mathrm{~Nm}\]The torque due to friction is \(2.5482 \mathrm{~Nm}\).

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 91Ó°ÊÓ!

Key Concepts

These are the key concepts you need to understand to accurately answer the question.

Linear Acceleration
Linear acceleration is a concept that describes how the velocity of an object changes with time along a straight path. In simpler terms, it tells us how quickly an object is speeding up or slowing down in a straight line. To find linear acceleration, we use the formula \[v^2 = u^2 + 2as\], where:
  • \(v\) is the final velocity. In our problem, the wheel comes to a stop, so \(v=0\) m/s.
  • \(u\) is the initial velocity. For our wheel, \(u = 43.0\) m/s.
  • \(s\) is the distance over which the wheel travels, which is 225 m in this case.
The equation is solved for \(a\), the linear acceleration, which gives us \(a = -4.11\) m/s². The negative sign indicates that the wheel is slowing down, which is also called deceleration. This helps us understand how fast the wheel's speed is decreasing until it stops.
Angular Acceleration
Angular acceleration is the rate at which the angular velocity of an object changes with time. For objects moving in a circle, this is an important concept because it helps us understand how quickly the object is rotating faster or slower. In this example, the angular acceleration \(\alpha\) is connected to the linear acceleration by the formula \(a = r\alpha\), where:
  • \(a\) is the linear acceleration, already found at 4.11 m/s².
  • \(r\) is the radius of the wheel, given as 0.250 m.
By rearranging the formula to solve for \(\alpha\), we have \(\alpha = \frac{a}{r}\), resulting in \(\alpha = 16.44\) rad/s². This tells us that for each meter per second squared of linear deceleration, the wheel's angular speed decreases more significantly due to its relatively small radius.
Torque
Torque is a measure of the rotational force applied to an object, causing it to rotate around an axis. It is similar to how force causes linear acceleration, but in this case, it brings about angular acceleration. In the context of this problem, torque due to friction is what slows the wheel down. The formula to find torque is \(\tau = I \alpha\), where:
  • \(\tau\) is the torque.
  • \(I\) is the rotational inertia of the object, which depends on how mass is distributed around the axis. In our problem, \(I = 0.155\) kg·m².
  • \(\alpha\) is the angular acceleration, previously determined to be 16.44 rad/s².
Using these values, we find the torque \(\tau = 2.5482\) Nm. This result shows the amount of rotational force needed to bring the wheel to a stop due to friction. Torque is a crucial concept in understanding how rotational motion is influenced by forces.

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

The rotational inertia of a collapsing spinning star drops to \(\frac{1}{3}\) its initial value. What is the ratio of the new rotational kinetic energy to the initial rotational kinetic energy?

A particle is acted on by two torques about the origin: \(\vec{\tau}_{1}\) has a magnitude of \(2.0 \mathrm{~N} \cdot \mathrm{m}\) and is directed in the positive direction of the \(x\) axis, and \(\vec{\tau}_{2}\) has a magnitude of \(4.0 \mathrm{~N} \cdot \mathrm{m}\) and is directed in the negative direçtion of the \(y\) axis. In unit-vector notation, find \(d \ell / d t,\) where \(\vec{\ell}\) is the angular momentum of the particle about the origin.

A constant horizontal force \(\vec{F}_{\text {app }}\) of magnitude \(12 \mathrm{~N}\) is applied to a uniform solid cylinder by fishing line wrapped around the cylinder. The mass of the cylinder is \(10 \mathrm{~kg},\) its radius is \(0.10 \mathrm{~m}\) and the cylinder rolls smoothly on the horizontal surface. (a) What is the magnitude of the acceleration of the center of mass of the cylinder? (b) What is the magnitude of the angular acceleration of the cylinder about the center of mass? (c) In unit-vector notation, what is the frictional force acting on the cylinder?

A uniform disk of mass \(10 m\) and radius \(3.0 r\) can rotate freely about its fixed center like a merry-go-round. A smaller uniform disk of mass \(m\) and radius \(r\) lies on top of the larger disk, concentric with it. Initially the two disks rotate together with an angular velocity of \(20 \mathrm{rad} / \mathrm{s}\). Then a slight disturbance causes the smaller disk to slide outward across the larger disk, until the outer edge of the smaller disk catches on the outer edge of the larger disk. Afterward, the two disks again rotate together (without further sliding). (a) What then is their angular velocity about the center of the larger disk? (b) What is the ratio \(K / K_{0}\) of the new kinetic energy of the twodisk system to the system's initial kinetic energy?

At time \(t=0,\) a \(3.0 \mathrm{~kg}\) particle with velocity \(\vec{v}=(5.0 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{i}}-(6.0 \mathrm{~m} / \mathrm{s}) \hat{\mathrm{j}}\) is at \(x=3.0 \mathrm{~m}, y=8.0 \mathrm{~m} .\) It is pulled by a \(7.0 \mathrm{~N}\) force in the negative \(x\) direction. About the origin, what are (a) the particle's angular momentum, (b) the torque acting on the particle, and (c) the rate at which the angular momentum is changing?

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.