A point on a rigid flywheel of radius 750 mm undergoes a uniform linear acceleration of 3 m/s2. The flywheel’s angular acceleration is
4 rad/s2
Understanding the relationship between linear acceleration and angular acceleration is fundamental in rotational dynamics, particularly for a rigid body like a flywheel. This problem requires us to determine the angular acceleration of a flywheel given the linear acceleration of a point on its rim and its radius.
For a point on a rigid body undergoing rotational motion, the linear acceleration (\(a\)) is directly proportional to the angular acceleration (\(\alpha\)) and the radial distance (\(r\)) from the axis of rotation to the point. The formula that connects these quantities is:
$$a = r \alpha$$
Where:
First, let's identify the information provided in the problem statement:
To perform calculations using standard SI units, we need to convert the radius from millimeters (mm) to meters (m). Since 1 meter (m) equals 1000 millimeters (mm):
$$r = 750 \, \text{mm} \times \frac{1 \, \text{m}}{1000 \, \text{mm}}$$
$$r = 0.750 \, \text{m}$$
Now, we can rearrange the relationship formula \(a = r \alpha\) to solve for the angular acceleration (\(\alpha\)):
$$\alpha = \frac{a}{r}$$
Substitute the given linear acceleration and the converted radius into this formula:
$$\alpha = \frac{3 \, \text{m/s}^2}{0.750 \, \text{m}}$$
Performing the division, we find the angular acceleration:
$$\alpha = 4 \, \text{rad/s}^2$$
Thus, the flywheel's angular acceleration is 4 rad/s\(\text{^2}\).
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