A photosensitive surface has work function \(\phi\). If photon of energy \(3 \phi\) falls on this surface, the electron comes out with maximum velocity of \(4 \times 10^6 \mathrm{~m} / \mathrm{s}\) When photon energy is increased to \(7 \phi\) then maximum velocity of photoelectron will be
\(4\sqrt{3}\times 10^{6}\text{ }\mathrm{m}/\mathrm{s}\)
\(2\sqrt{3}\times 10^{6}\text{ }\mathrm{m}/\mathrm{s}\)
\(4\sqrt{3}\times 10^{3}\text{ }\mathrm{m}/\mathrm{s}\)
\(2\sqrt{3}\times 10^{3}\text{ }\mathrm{m}/\mathrm{s}\)
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.