/*! 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 96 A \(55-\mathrm{kg}\) runner runs... [FREE SOLUTION] | 91Ó°ÊÓ

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A \(55-\mathrm{kg}\) runner runs around the edge of a horizontal turntable mounted on a vertical, frictionless axis through its center. The runner's velocity relative to the earth has magnitude 2.8 \(\mathrm{m} / \mathrm{s}\) . The turntable is rotating in the opposite direction with an angular velocity of magnitude 0.20 \(\mathrm{rad} / \mathrm{s}\) relative to the earth. The radius of the turntable is \(3.0 \mathrm{m},\) and its moment of inertia about the axis of rotation is 80 \(\mathrm{kg} \cdot \mathrm{m}^{2} .\) Find the final angular velocity of the system if the runner comes to rest relative to the turntable. (You can model the runner as a particle.)

Short Answer

Expert verified
The final angular velocity of the system is approximately 0.776 rad/s.

Step by step solution

01

Understand the Conservation of Angular Momentum

The angular momentum of a system is conserved when no external torques act on it. In this problem, we're tasked with finding the final angular velocity of a system where initially, the runner and turntable have initial angular momentum and the turntable has some moment of inertia. The initial angular momentum of the runner and turntable should equal the final angular momentum of the combined system as the runner comes to rest relative to the turntable.
02

Calculate the Initial Angular Momentum of the Runner

The runner can be considered a particle moving along the edge of the turntable, so its initial angular momentum can be calculated by the formula \( L_{runner} = m imes v imes r \), where \( m = 55 \,\text{kg} \) is the mass of the runner, \( v = 2.8 \,\text{m/s} \) is their initial velocity, and \( r = 3.0 \,\text{m} \) is the radius of the turntable. Thus, \( L_{runner} = 55 \,\text{kg} \times 2.8 \,\text{m/s} \times 3.0 \,\text{m} = 462 \,\text{kg} \cdot \text{m}^2/\text{s} \).
03

Calculate the Initial Angular Momentum of the Turntable

The initial angular momentum of the turntable, rotating in the opposite direction, is given similarly by \( L_{turntable} = I \times \omega \), where \( I = 80 \,\text{kg} \cdot \text{m}^2 \) is the moment of inertia, and \( \omega = -0.20 \,\text{rad/s} \) is the angular velocity (negative as it is in the opposite direction). Thus, \( L_{turntable} = 80 \,\text{kg} \cdot \text{m}^2 \times (-0.20 \,\text{rad/s}) = -16 \,\text{kg} \cdot \text{m}^2/\text{s} \).
04

Combine the Angular Momenta for Conservation

The total initial angular momentum \( L_{initial} \) is the sum of the angular momentum of the runner and the turntable: \( L_{initial} = 462 \,\text{kg} \cdot \text{m}^2/\text{s} - 16 \,\text{kg} \cdot \text{m}^2/\text{s} = 446 \,\text{kg} \cdot \text{m}^2/\text{s} \). In the final state, the system's angular momentum must equal this initial total because of conservation.
05

Calculate the Final Angular Velocity

Now consider the final system: the total moment of inertia \( I_{total} \) is the sum of the turntable's and the effective moment of inertia of the runner, calculated as if the runner is resting relative to the turntable: \( I_{total} = 80 + 55 \times 3^2 = 80 + 495 = 575 \,\text{kg} \cdot \text{m}^2 \). If \( \omega_{final} \) is the final angular velocity, conservation of angular momentum gives \( 575 \,\text{kg} \cdot \text{m}^2 \cdot \omega_{final} = 446 \,\text{kg} \cdot \text{m}^2/\text{s} \). Solving for \( \omega_{final} \), we find \( \omega_{final} = \frac{446}{575} \approx 0.776 \,\text{rad/s} \).

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Key Concepts

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

Angular Velocity
Angular velocity is a critical concept in understanding rotational systems. It represents how quickly an object rotates or spins around an axis. Unlike linear velocity, which measures how fast an object moves from one point to another, angular velocity focuses on circular motion. It is expressed in radians per second (\( ext{rad/s} \)).

To visualize angular velocity, imagine how fast the hands of a clock rotate. The hour hand moves slower compared to the minute hand, demonstrating different angular velocities. In this exercise, the turntable has an initial angular velocity of \(-0.20 \text{ rad/s}\), rotating in the opposite direction of the runner's motion.

Angular velocity is a vector quantity, meaning it has both magnitude and direction. The direction indicates whether the rotation is clockwise or counterclockwise. In problems involving angular motion, understanding these directions and magnitudes is crucial for solving equations and applying principles effectively.
Moment of Inertia
The moment of inertia is akin to mass in linear motion but for rotational systems. It measures an object's resistance to changes in its rotational state. The larger the moment of inertia, the harder it is to change the object's rotation. This is why heavier objects or those with their mass distributed further from the axis are harder to spin.

Mathematically, the moment of inertia \( I \) can be expressed as \( I = mr^2 \) for point masses, where \( m \) is the mass and \( r \) is the distance from the axis of rotation. In our exercise, the turntable's moment of inertia is given as \( 80 \, \text{kg} \cdot \text{m}^2 \).
  • It plays a central role in calculating angular momentum and solving dynamics problems.
  • Understanding how inertia influences motion helps in making sense of rotational dynamics.
Moment of inertia varies depending on the object's shape and mass distribution. This property underpins many real-world applications, from designing machinery to understanding planetary motion.
Physics Education
The exploration of angular momentum and rotational dynamics is crucial in physics education. These concepts help students understand how objects move and interact in different ways than linear motion. By studying rotational motion, students gain insights into how everyday objects operate, from spinning tops to orbiting satellites.

Physics education often includes hands-on experiments and real-life applications to demystify these concepts. For students, this exercise is an opportunity to see the principles of angular momentum conservation in action. Incorporating technology and simulations can also enhance understanding, providing visual insights into how rotational forces play out.
  • Interactive tools and experiments make the learning process engaging.
  • Theoretical problems like this one help bridge the gap to practical application.
Understanding these fundamentals prepares students for more advanced studies in physics and related fields.
Rotational Motion
Rotational motion is a type of movement where an object rotates around an axis. It's a fundamental concept in physics, playing a crucial role in various physical theories and applications. When studying rotational motion, several key quantities are considered:
  • Angular Displacement: The angle through which an object rotates, measured in radians.
  • Angular Velocity: As mentioned, it is how quickly an object rotates, measured in \( \text{rad/s} \).
  • Angular Acceleration: The rate of change of angular velocity, telling us how an object's speed of rotation increases or decreases.
In our exercise, the rotational motion consists of both the turntable and the runner. This interaction involving the runner stopping relative to the turntable illustrates how rotational dynamics govern systems with multiple moving parts.

Applications of rotational motion are widespread, from everyday items like wheels and gears to the vast rotations of celestial bodies. Understanding how these elements work in harmony or opposition provides the foundation for fields such as engineering, astronomy, and even biomechanics.

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Most popular questions from this chapter

The engine delivers 175 hp to an aircraft propeller at 2400 rev/min. (a) How much torque does the aircraft engine provide? (b) How much work does the engine do in one revolution of the propeller?

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The Yo-yo. A yo-yo is made from two uniform disks, each with mass \(m\) and radius \(R\) , connected by a light axle of radius b. A light, thin string is wound several times around the axle and then held stationary while the yo-yo is released from rest, dropping as the string unwinds. Find the linear acceleration and angular acceleration of the yo-yo and the tension in the string.

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