The stopping potential \( V_0 \) is related to the maximum kinetic energy of the emitted photoelectrons through the equation:
\( KE_{\text{max}} = h\nu - \phi_0 = eV_0, \)
where:
- \( h \) is Planck’s constant,
- \( \nu \) is the frequency of the incident light,
- \( \phi_0 \) is the work function of the emitter material,
- \( e \) is the elementary charge.
Key points to note:
1. The stopping potential \( V_0 \) depends on the frequency of the incident light (\( \nu \)) but is independent of the intensity of the light. Increasing the intensity of the incident light increases the number of emitted photoelectrons but does not affect their maximum kinetic energy or the stopping potential.
2. The stopping potential is also influenced by the nature of the emitter material since different materials have different work functions (\( \phi_0 \)).
Therefore, statement (3) is incorrect, as \( V_0 \) does not increase with an increase in the intensity of the incident light.
A black body is at a temperature of 2880 K. The energy of radiation emitted by this body with wavelength between 499 nm and 500 nm is U1, between 999 nm and 1000 nm is U2 and between 1499 nm and 1500 nm is U3. The Wien's constant, b = 2.88×106 nm-K. Then,


What will be the equilibrium constant of the given reaction carried out in a \(5 \,L\) vessel and having equilibrium amounts of \(A_2\) and \(A\) as \(0.5\) mole and \(2 \times 10^{-6}\) mole respectively?
The reaction : \(A_2 \rightleftharpoons 2A\)