The maximum height \( H \) attained by a projectile is given by the formula: \[ H = \frac{u^2 \sin^2(\theta)}{2g}, \] where: - \( u \) is the initial velocity, - \( \theta \) is the angle of projection, - \( g \) is the acceleration due to gravity.
Case 1: Original values In the first case, let the initial velocity be \( u \) and the angle of projection be \( \theta \). The maximum height attained in the first case is: \[ H_1 = \frac{u^2 \sin^2(\theta)}{2g}. \]
Case 2: Doubled mass and angle In the second case, the mass is doubled, but the initial velocity remains the same. The angle of projection is also doubled, so the angle becomes \( 2\theta \). The maximum height in the second case is: \[ H_2 = \frac{u^2 \sin^2(2\theta)}{2g}. \] Using the double angle identity for sine, we know that: \[ \sin(2\theta) = 2 \sin(\theta) \cos(\theta). \]
Thus, the maximum height in the second case becomes: \[ H_2 = \frac{u^2 \left(2 \sin(\theta) \cos(\theta)\right)^2}{2g} = \frac{4u^2 \sin^2(\theta) \cos^2(\theta)}{2g}. \]
Now, the ratio of the maximum heights in the first case to the second case is: \[ \frac{H_1}{H_2} = \frac{\frac{u^2 \sin^2(\theta)}{2g}}{\frac{4u^2 \sin^2(\theta) \cos^2(\theta)}{2g}} = \frac{1}{4 \cos^2(\theta)}. \] For \( \theta = 30^\circ \), \( \cos(30^\circ) = \frac{\sqrt{3}}{2} \), so: \[ \frac{H_1}{H_2} = \frac{1}{4 \left(\frac{\sqrt{3}}{2}\right)^2} = \frac{1}{4 \times \frac{3}{4}} = \frac{1}{3}. \]
Thus, the ratio of the maximum heights attained is \( 1 : 3 \), and the correct answer is option (C).
A solid cylinder of mass 2 kg and radius 0.2 m is rotating about its own axis without friction with angular velocity 5 rad/s. A particle of mass 1 kg moving with a velocity of 5 m/s strikes the cylinder and sticks to it as shown in figure.
The angular velocity of the system after the particle sticks to it will be: