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During the launch from a board, a diver's angular speed about her center of mass changes from zero to \(6.20 \mathrm{rad} / \mathrm{s}\) in \(220 \mathrm{~ms}\). Her rotational inertia about her center of mass is \(12.0 \mathrm{~kg} \cdot \mathrm{m}^{2} .\) During the launch, what are the magnitudes of (a) her average angular acceleration and (b) the average external torque on her from the board?

Short Answer

Expert verified
(a) Average angular acceleration is 28.18 rad/s². (b) Average external torque is 338.16 N·m.

Step by step solution

01

Identify Known Values

First, list the given values from the problem: The initial angular speed is \(\omega_{i} = 0\, \text{rad/s}\), the final angular speed is \(\omega_{f} = 6.20\, \text{rad/s}\), and the time interval is \(t = 220\, \text{ms} = 0.220\, \text{s}\). The rotational inertia is \(I = 12.0\, \text{kg} \cdot \text{m}^2\).
02

Calculate Average Angular Acceleration

Use the formula for average angular acceleration: \(\alpha = \frac{\omega_{f} - \omega_{i}}{t}\). Substitute the known values to find \(\alpha = \frac{6.20 - 0}{0.220} = 28.18\, \text{rad/s}^2\).
03

Calculate Average External Torque

Use the relationship between torque, rotational inertia, and angular acceleration: \(\tau = I \cdot \alpha\). Substitute \(I = 12.0\, \text{kg} \cdot \text{m}^2\) and \(\alpha = 28.18\, \text{rad/s}^2\) to find \(\tau = 12.0 \times 28.18 = 338.16\, \text{N} \cdot \text{m}\).

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Key Concepts

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

Angular Speed
Think of angular speed as the rotational version of linear speed. It describes how fast an object is rotating. Angular speed is usually measured in radians per second (\(\text{rad/s}\)). For instance, in our example, the diver's angular speed changes from zero to 6.20 rad/s. This means she starts from a stationary position and reaches a higher speed as she spins.

The formula for angular speed is:\[\omega = \frac{\theta}{t}\]where \(\omega\) is the angular speed, \(\theta\) is the angle of rotation in radians, and \(t\) is the time it takes to rotate through that angle. In our scenario, however, we already had the initial and final angular speeds to determine the angular acceleration. Here are some key points about angular speed:
  • It does not depend on the direction of spin; it only quantifies how fast the rotation happens.
  • Angular speed helps us understand how quickly an object like a diver spins or rotates around a fixed axis.
Changes in angular speed often occur due to external influences, like the diver's push-off from the board.
Rotational Inertia
Rotational inertia, also known as the moment of inertia, reflects how difficult it is to change the rotational state of an object. It's akin to mass in linear motion. For objects that rotate, it describes how the mass is distributed relative to the axis of rotation. The diver in our example has a rotational inertia of 12.0 kg·m² about her center of mass.

In layman's terms, a larger rotational inertia means more effort is needed to change the rotational speed, whether that means spinning faster or slower. Here's what is critical about rotational inertia:
  • It's determined by both the amount of mass and how far that mass is from the rotation axis.
  • Different shapes and mass distributions create different rotational inertias, even for the same total mass.
  • For example, divers tuck their limbs in to rotate faster, which effectively reduces their rotational inertia.
Understanding rotational inertia is pivotal for divers as they change their body positions during dives to control their spins effectively.
External Torque
Torque is the measure of how much a force acting on an object causes that object to rotate. Think of it as a rotational equivalent of force. When the diver launches from the board, an external torque is applied to accelerate her rotation. In our exercise, this torque was found to be 338.16 N·m.

The formula connecting torque \(\tau\), rotational inertia \(I\), and angular acceleration \(\alpha\) is:\[\tau = I \cdot \alpha\]
  • \(I\) represents the rotational inertia.
  • \(\alpha\) is the angular acceleration, which highlights how quickly the angular speed changes.
  • Torque attempts to increase or decrease the angular speed of an object around a pivot point.
By applying torque, forces like those from a diving board generate angular motion. This principle is crucial for all rotating bodies, highlighting the relationship between force applied and rotational speed.

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Most popular questions from this chapter

A gyroscope flywheel of radius \(2.83 \mathrm{~cm}\) is accelerated from rest at \(14.2 \mathrm{rad} / \mathrm{s}^{2}\) until its angular speed is \(2760 \mathrm{rev} / \mathrm{min} .\) (a) What is the tangential acceleration of a point on the rim of the flywheel during this spin-up process? (b) What is the radial acceleration of this point when the flywheel is spinning at full speed? (c) Through what distance does a point on the rim move during the spin-up?

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