To find the angular acceleration, we use the formula for uniform angular acceleration: \(\alpha = \frac{\Delta \omega}{\Delta t}\), where \(\Delta \omega\) is the change in angular velocity and \(\Delta t\) is the change in time.
Given:
First, convert angular speeds from rpm to rad/s using the conversion factor \(1 \text{ rpm} = \frac{2\pi}{60} \text{ rad/s}\):
\(\omega_i = 1200 \times \frac{2\pi}{60} = 40\pi \text{ rad/s}\)
\(\omega_f = 3120 \times \frac{2\pi}{60} = 104\pi \text{ rad/s}\)
The change in angular velocity, \(\Delta \omega = \omega_f - \omega_i = 104\pi - 40\pi = 64\pi \text{ rad/s}\)
Now, using the formula for angular acceleration:
\(\alpha = \frac{\Delta \omega}{\Delta t}\)
\(\alpha = \frac{64\pi}{16} = 4\pi \text{ rad/s}^2\)
Therefore, the angular acceleration is \(4\pi \text{ rad/s}^2\).
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.
AB is a part of an electrical circuit (see figure). The potential difference \(V_A - V_B\), at the instant when current \(i = 2\) A and is increasing at a rate of 1 amp/second is:
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: