
By impulse β momentum theorem: \( J = M V_{CM} \)
Therefore, the center of mass velocity \( V_{CM} \) is: \[ V_{CM} = \frac{J}{M} = \frac{\frac{\pi}{2}}{100 \times \frac{5}{1000}} = \sqrt{2\pi} \]
The total time of the journey is: \[ \Delta t = \frac{\sqrt{2\pi}}{5} \]
By the angular impulse-momentum theorem: \[ J \times \frac{R}{2} = \left[\frac{M R^2}{4}\right] w \]
Solving for the angular velocity \( w \): \[ w = \frac{J \times \frac{R}{2}}{\frac{M R^2}{4}} = \frac{J}{M R} \times 2 \]
Substituting the known values: \[ w = \frac{\frac{\frac{\sqrt{\pi}}{2}}{100} \times 2}{\frac{5}{1000} \times \frac{4}{3} \times \frac{1}{100}} = 2 \times 75 \sqrt{2\pi} \, \text{rad/s} \]
The number of rotations is: \[ n = \frac{w \times \Delta t}{2\pi} = 30 \]
Therefore, the final result is: \[ n = 30 \]
A wheel of radius $ 0.2 \, \text{m} $ rotates freely about its center when a string that is wrapped over its rim is pulled by a force of $ 10 \, \text{N} $. The established torque produces an angular acceleration of $ 2 \, \text{rad/s}^2 $. Moment of inertia of the wheel is............. kg mΒ².
The reaction sequence given below is carried out with 16 moles of X. The yield of the major product in each step is given below the product in parentheses. The amount (in grams) of S produced is ____. 
Use: Atomic mass (in amu): H = 1, C = 12, O = 16, Br = 80
Let $ \mathbb{R} $ denote the set of all real numbers. Then the area of the region $$ \left\{ (x, y) \in \mathbb{R} \times \mathbb{R} : x > 0, y > \frac{1}{x},\ 5x - 4y - 1 > 0,\ 4x + 4y - 17 < 0 \right\} $$ is
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ 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: