We have two rotational velocities:
\(ω_1\), which is 1200 revolutions per minute, and \(ω_2\), which is 3120 revolutions per minute.
We also know that the time it takes for the rotation to go from \(ω_1\) to \(ω_2\) is 16 seconds.
Using this information, we can calculate the angular acceleration \((\alpha)\) of the rotation as follows:
\(\alpha = [\frac{(ω_2 - ω_1)}{t}] \times [\frac{2\pi}{60}]\)
\(\alpha = [\frac{(3120 - 1200)}{16}] \times [\frac{2\pi}{60}]\)
\(\alpha = (\frac{1920}{16}) \times (\frac{2\pi}{60})\)
\(\alpha = 4\pi\)
Therefore, the angular acceleration is 4π radians per second squared.
A uniform circular disc of radius \( R \) and mass \( M \) is rotating about an axis perpendicular to its plane and passing through its center. A small circular part of radius \( R/2 \) is removed from the original disc as shown in the figure. Find the moment of inertia of the remaining part of the original disc about the axis as given above.
Rotational motion can be defined as the motion of an object around a circular path, in a fixed orbit.
The wheel or rotor of a motor, which appears in rotation motion problems, is a common example of the rotational motion of a rigid body.
Other examples: