Problem 14
Question
A circular saw blade 0.200 \(\mathrm{m}\) in diameter starts from rest. In 6.00 \(\mathrm{s}\) , it reaches an angular velocity of 140 \(\mathrm{rad} / \mathrm{s}\) with constant angular acceleration. Find the angular acceleration and the angle through which the blade has turned in this time.
Step-by-Step Solution
Verified Answer
Angular acceleration is 23.33 rad/s²; the blade turns 419.94 radians.
1Step 1: Understand the Problem
Identify what is given and what needs to be found. The blade starts from rest, has a diameter of 0.200 meters, and reaches an angular velocity of 140 rad/s in 6.00 seconds under constant angular acceleration. We need to find the angular acceleration (\(\alpha\)) and the angle (\(\theta\)) through which the blade has turned.
2Step 2: Convert Linear Diameter to Radius
Convert the diameter into radius since the radius is needed for angular formulas. \[ r = \frac{d}{2} = \frac{0.200}{2} = 0.100 \text{ m} \]
3Step 3: Use Angular Kinematics Formula for Angular Acceleration
Use the angular kinematics formula: \( \omega_f = \omega_i + \alpha t \). Given initial angular velocity \( \omega_i = 0 \) (rad/s) and final angular velocity \( \omega_f = 140 \) (rad/s) with time \( t = 6.00 \) (s), solve for angular acceleration \( \alpha \):\[ 140 = 0 + \alpha \times 6.00 \]\[ \alpha = \frac{140}{6.00} = 23.33 \text{ rad/s}^2 \]
4Step 4: Use Formula to Find the Angle of Rotation
Use the formula for angular displacement: \( \theta = \omega_i t + \frac{1}{2} \alpha t^2 \). With \( \omega_i = 0 \) (rad/s), \( \alpha = 23.33 \) (rad/s²), solve for \( \theta \):\[ \theta = 0 \times 6.00 + \frac{1}{2} \times 23.33 \times (6.00)^2 \]\[ \theta = \frac{1}{2} \times 23.33 \times 36.00 \]\[ \theta = 419.94 \text{ rad} \]
5Step 5: Conclusion
The angular acceleration is \( 23.33 \text{ rad/s}^2 \) and the blade turns through \( 419.94 \text{ radians}\).
Key Concepts
Angular AccelerationAngular DisplacementAngular Velocity
Angular Acceleration
Angular acceleration is a key concept in understanding how quickly an object's rotational speed changes over time. It's like a version of linear acceleration but for rotating objects. To find angular acceleration, use the formula:
Angular acceleration is measured in "radians per second squared" or \( \text{rad/s}^2 \).
When solving the exercise, the blade starts from rest, which means \( \omega_i = 0 \) rad/s. The blade reaches 140 rad/s in 6 seconds, so \( \omega_f = 140 \) rad/s and \( t = 6 \) s. Plugging these into the formula, the calculated angular acceleration is \( 23.33 \text{ rad/s}^2 \).
This means the blade's speed increases at a constant rate of 23.33 radians for every second squared.
- \( \alpha = \frac{\omega_f - \omega_i}{t} \)
Angular acceleration is measured in "radians per second squared" or \( \text{rad/s}^2 \).
When solving the exercise, the blade starts from rest, which means \( \omega_i = 0 \) rad/s. The blade reaches 140 rad/s in 6 seconds, so \( \omega_f = 140 \) rad/s and \( t = 6 \) s. Plugging these into the formula, the calculated angular acceleration is \( 23.33 \text{ rad/s}^2 \).
This means the blade's speed increases at a constant rate of 23.33 radians for every second squared.
Angular Displacement
Angular displacement is the measure of the angle through which an object has rotated during a certain period. It is the rotational equivalent of the distance traveled in linear motion. The formula for calculating angular displacement \( \theta \) when starting from rest is:
This value is derived from the calculation:
- \( \theta = \omega_i t + \frac{1}{2} \alpha t^2 \)
This value is derived from the calculation:
- \( \theta = \frac{1}{2} \times 23.33 \times 36 \)
Angular Velocity
Angular velocity describes how fast an object rotates or spins around an axis. It is defined as the rate of change of angular displacement and is measured in radians per second (rad/s).
Angular velocity can be thought of as the speed of rotation. There are two types: initial angular velocity (\( \omega_i \)) and final angular velocity (\( \omega_f \)).
Understanding this concept is vital for solving problems involving rotational motion.
Angular velocity can be thought of as the speed of rotation. There are two types: initial angular velocity (\( \omega_i \)) and final angular velocity (\( \omega_f \)).
- In our exercise, since the blade starts from rest, the initial angular velocity \( \omega_i \) is 0 rad/s.
- After 6 seconds of applying a constant angular acceleration, the blade reaches a final angular velocity \( \omega_f \), calculated as 140 rad/s.
Understanding this concept is vital for solving problems involving rotational motion.
Other exercises in this chapter
Problem 12
\(\cdot\) When the power is turned off on a turntable spinning at 78.0 rpm, you find that it takes 10.5 revolutions for it to stop while slowing down at a unifo
View solution Problem 13
DVDs. The angular speed of digital video discs (DVDs) varies with whether the inner or outer part of the disc is being read. (CDs function in the same way.) Ove
View solution Problem 15
\(\cdot\) A wheel turns with a constant angular acceleration of 0.640 \(\mathrm{rad} / \mathrm{s}^{2} .\) (a) How much time does it take to reach an angular vel
View solution Problem 16
An electric fan is turned off, and its angular velocity decreases uniformly from 500.0 rev/min to 200.0 rev/min in 4.00 s. (a) Find the angular acceleration in
View solution