Two identical photocathodes receive light of frequencies ' \(f 1\) ' and ' \(f_2\) '. The velocity of the photoelectrons of mass ' \(m\) ' emitted are respectively ' \(\mathrm{v}_1\) ' and ' \(\mathrm{v}_2\) '. Then the correct relation is ( \(\mathrm{h}=\) Planck's constant)
\(v_{1}-v_{2}=[\frac{2h}{m}(f_{1}-f_{2})]^{\frac{1}{2}}\)
\(v_{1}+v_{2}=[\frac{2h}{m}(f_{1}+f_{2})]^{\frac{1}{2}}\)
\(v_{1}^{2}-v_{2}^{2}=\frac{2h}{m}(f_{1}-f_{2})\)
\(v_{1}^{2}+v_{2}^{2}=\frac{2h}{m}(f_{1}+f_{2})\)
In a photoelectric effect experiment, light of wavelength \( \lambda \), \( \lambda/2 \), and \( \lambda/6 \) are incident on a metal surface. The stopping potential for these wavelengths are given as \( V_1 \), \( V_2 \), and \( V_3 \), respectively. If the work function of the metal is \( \phi \), calculate the work function using the given wavelengths. The photoelectric equation is given by: \[ E_k = h \nu - \phi \] where:
\( E_k \) is the kinetic energy of the emitted electrons (which is related to the stopping potential),
\( h \) is Planck's constant,
\( \nu \) is the frequency of the incident light,
\( \phi \) is the work function of the metal.
The frequency \( \nu \) is related to the wavelength \( \lambda \) by the equation: \[ \nu = \frac{c}{\lambda} \] where \( c \) is the speed of light.