The photoelectric current is dependent on two factors:
1. The intensity of the light (\( I \)), which is proportional to the number of photons striking the surface.
2. The frequency of the light (\( \nu \)), which must be above the threshold frequency \( \nu_0 \) to cause emission of photoelectrons. The energy of a photon is given by: \[ E_{\text{photon}} = h \nu, \] where \( h \) is Planck's constant and \( \nu \) is the frequency of the light. For photoelectric emission to occur, the frequency \( \nu \) must be greater than or equal to the threshold frequency \( \nu_0 \). In this case, the frequency of the light is \( \frac{11}{6} \nu_0 \), which is above the threshold frequency, so photoelectric emission occurs.
Step 1: Halving the frequency
When the frequency is halved, the new frequency becomes \( \frac{1}{2} \times \frac{11}{6} \nu_0 = \frac{11}{12} \nu_0 \). This new frequency is below the threshold frequency \( \nu_0 \), which means that the light will no longer have enough energy to emit photoelectrons.
Step 2: Effect on the photoelectric current
Since the frequency is now below the threshold frequency, no photoelectrons will be emitted, and therefore the photoelectric current \( I_1 \) will be zero.
Thus, the new photoelectric current is \( I_1 = 0 \).
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: