Step 1: Define angular momentum. The angular momentum at maximum height is expressed as: \[ L = m v H \] where \( H \) represents the maximum height.
Step 2: Determine the horizontal velocity. The horizontal velocity component is constant: \[ v = u \cos 30^\circ = u \times \frac{\sqrt{3}}{2} \]
Step 3: Calculate the maximum height. Employing the kinematic equation: \[ H = \frac{u^2 \sin^2 30^\circ}{2g} \] With \( \sin 30^\circ = \frac{1}{2} \), this simplifies to: \[ H = \frac{u^2 \times \left(\frac{1}{2}\right)^2}{2g} = \frac{u^2}{8g} \]
Step 4: Compute angular momentum. Substitute the expressions for velocity and height: \[ L = m u \cos 30^\circ \times H \] \[ = m u \times \frac{\sqrt{3}}{2} \times \frac{u^2}{8g} \] \[ = \frac{\sqrt{3} m u^3}{16 g} \] The final result is (A) \( \frac{\sqrt{3}}{16} \frac{m u^3}{g} \).
When a photon of suitable frequency is incident on a metal surface, a photoelectron is emitted from it. If the frequency is below a threshold frequency (ν0) for the surface, no photoelectron is emitted. For a photon of frequency ν (ν > ν0), the kinetic energy of the emitted photoelectron is:
Km = h(ν − ν0)
The photocurrent can be stopped by applying a potential V0, called the "stopping potential," on the anode. Thus, the maximum kinetic energy of photoelectrons is:
Km = eV0 = h(ν − ν0)
The experimental graph between V0 and ν for a metal is shown in the figure. This is a straight line of slope m.