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

A 2.00 -kg thin hoop with a 50.0 -cm radius rolls down a \(30.0^{\circ}\) slope without slipping. If the hoop starts from rest at the top of the slope, what is its translational velocity after it rolls \(10.0 \mathrm{~m}\) along the slope?

Short Answer

Expert verified
Answer: The translational velocity of the hoop is approximately 4.95 m/s.

Step by step solution

01

Identify the initial and final energies

Initially, the hoop is at rest at the top of the slope, so it only has gravitational potential energy, which we'll denote as PE_1. After rolling down 10 meters along the slope, it will have both kinetic and gravitational potential energy, which we'll denote as KE_2 and PE_2.
02

Determine the change in height

To determine the change in height, we'll use trigonometry. From the slope angle, we can set up a right triangle. The change in height, Δh, can be found using the sine function: \(\Delta h = L \sin{θ}\) where L is the distance the hoop rolls along the slope and θ is the angle of the slope. Plugging in the given values: \(\Delta h = 10 \mathrm{~m} \times \sin{30^{\circ}} = 5 \mathrm{~m}\)
03

Calculate the initial and final energies

Next, we can calculate the initial potential energy (PE_1) and the final potential and kinetic energies (PE_2 and KE_2). The gravitational potential energy can be found using the formula: \(PE = mgh\) where m is the mass of the hoop, g is the acceleration due to gravity (9.81 m/s²), and h is the height. \(PE_1 = (2.00 \mathrm{~kg}) \times (9.81 \mathrm{~m/s^2}) \times (5 \mathrm{~m}) = 98.1 \mathrm{~J}\) Now, we can find the final potential energy (PE_2): \(PE_2 = (2.00 \mathrm{~kg}) \times (9.81 \mathrm{~m/s^2}) \times (0 \mathrm{~m}) = 0 \mathrm{~J}\) Since the hoop rolls without slipping, the total kinetic energy (KE_2) can be divided into translational and rotational components. For a thin hoop, the rotational kinetic energy is: \(KE_\text{rotational} = \frac{1}{2}I\omega^2\) where I is the moment of inertia of the thin hoop, which is given by: \(I = mr^2\) and ω is the angular velocity, which is related to the translational velocity v by: \(\omega = \frac{v}{r}\) The translational kinetic energy is given by: \(KE_\text{translational} = \frac{1}{2}mv^2\) Therefore, the total kinetic energy (KE_2) is: \(KE_2 = KE_\text{translational} + KE_\text{rotational} = \frac{1}{2}mv^2 + \frac{1}{2}(mr^2)\left(\frac{v}{r}\right)^2\)
04

Use conservation of mechanical energy

According to the conservation of mechanical energy, the initial total energy (PE_1) is equal to the final total energy (PE_2 + KE_2): \(PE_1 = PE_2 + KE_2\) Substituting the expressions for PE_1, PE_2, and KE_2: \(98.1 \mathrm{~J} = 0 + \left[\frac{1}{2}(2.00 \mathrm{~kg})v^2 + \frac{1}{2}(2.00 \mathrm{~kg})(0.5 \mathrm{~m})^2\left(\frac{v}{0.5 \mathrm{~m}}\right)^2\right]\) Now, we can simplify and solve for v: \(98.1 \mathrm{~J} = mv^2 + mv^2\) \(98.1 \mathrm{~J} = 2mv^2\) \(v^2 = \frac{98.1 \mathrm{~J}}{4.00 \mathrm{~kg}}\) \(v = \sqrt{\frac{98.1 \mathrm{~J}}{4.00 \mathrm{~kg}}} = \frac{\sqrt{98.1 \mathrm{~J}}}{\sqrt{4.00 \mathrm{~kg}}} \approx 4.95 \mathrm{~m/s}\) So, the translational velocity of the hoop after it has traveled 10 meters along the slope is approximately 4.95 m/s.

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 wagon wheel is made entirely of wood. Its components consist of a rim, 12 spokes, and a hub. The rim has mass \(5.2 \mathrm{~kg}\), outer radius \(0.90 \mathrm{~m}\), and inner radius \(0.86 \mathrm{~m}\). The hub is a solid cylinder with mass \(3.4 \mathrm{~kg}\) and radius \(0.12 \mathrm{~m} .\) The spokes are thin rods of mass \(1.1 \mathrm{~kg}\) that extend from the hub to the inner side of the rim. Determine the constant \(c=I / M R^{2}\) for this wagon wheel.

It is harder to move a door if you lean against it (along the plane of the door) toward the hinge than if you lean against the door perpendicular to its plane. Why is this so?

A space station is to provide artificial gravity to support long-term stay of astronauts and cosmonauts. It is designed as a large wheel, with all the compartments in the rim, which is to rotate at a speed that will provide an acceleration similar to that of terrestrial gravity for the astronauts (their feet will be on the inside of the outer wall of the space station and their heads will be pointing toward the hub). After the space station is assembled in orbit, its rotation will be started by the firing of a rocket motor fixed to the outer rim, which fires tangentially to the rim. The radius of the space station is \(R=50.0 \mathrm{~m},\) and the mass is \(M=2.40 \cdot 10^{5} \mathrm{~kg} .\) If the thrust of the rocket motor is \(F=1.40 \cdot 10^{2} \mathrm{~N},\) how long should the motor fire?

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 circular platform of radius \(R_{p}=4.00 \mathrm{~m}\) and mass \(M_{\mathrm{p}}=400 .\) kg rotates on frictionless air bearings about its vertical axis at 6.00 rpm. An 80.0 -kg man standing at the very center of the platform starts walking \((\) at \(t=0)\) radially outward at a speed of \(0.500 \mathrm{~m} / \mathrm{s}\) with respect to the platform. Approximating the man by a vertical cylinder of radius \(R_{\mathrm{m}}=0.200 \mathrm{~m}\) determine an equation (specific expression) for the angular velocity of the platform as a function of time. What is the angular velocity when the man reaches the edge of the platform?

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