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.
A sphere of radius R is cut from a larger solid sphere of radius 2R as shown in the figure. The ratio of the moment of inertia of the smaller sphere to that of the rest part of the sphere about the Y-axis is :
The current passing through the battery in the given circuit, is:
A bob of heavy mass \(m\) is suspended by a light string of length \(l\). The bob is given a horizontal velocity \(v_0\) as shown in figure. If the string gets slack at some point P making an angle \( \theta \) from the horizontal, the ratio of the speed \(v\) of the bob at point P to its initial speed \(v_0\) 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: