The photoelectric work function of the metal is given as \( 2.4 \, \text{eV} \). The energy of a photon is related to its wavelength by the equation: \[ E = \frac{hc}{\lambda} \] where:
\( E \) is the energy of the photon in electron volts (eV),
\( h \) is Planck's constant (\( 6.626 \times 10^{-34} \, \text{J} \cdot \text{s} \)),
\( c \) is the speed of light (\( 3 \times 10^8 \, \text{m/s} \)),
\( \lambda \) is the wavelength in meters. The photoemission will not take place unless the energy of the incident photon is greater than or equal to the work function of the metal. The energy corresponding to each wavelength is calculated using the above equation. For each wavelength, we compare the photon energy to the work function of \( 2.4 \, \text{eV} \).
For \( \lambda = 200 \, \text{nm} \), \[ E = \frac{(6.626 \times 10^{-34}) (3 \times 10^8)}{200 \times 10^{-9}} = 6.626 \, \text{eV} > 2.4 \, \text{eV} \] Photon energy is greater than the work function, so photoemission occurs.
For \( \lambda = 300 \, \text{nm} \), \[ E = 4.14 \, \text{eV} > 2.4 \, \text{eV} \] Photon energy is greater than the work function, so photoemission occurs.
For \( \lambda = 400 \, \text{nm} \), \[ E = 3.1 \, \text{eV} > 2.4 \, \text{eV} \] Photon energy is greater than the work function, so photoemission occurs.
For \( \lambda = 700 \, \text{nm} \), \[ E = 1.77 \, \text{eV} < 2.4 \, \text{eV} \] Photon energy is less than the work function, so photoemission does not occur. Thus, the wavelength for which photoemission does not take place is \( 700 \, \text{nm} \). Thus, the solution is \( 700 \, \text{nm} \).
A sub-atomic particle of mass \( 10^{-30} \) kg is moving with a velocity of \( 2.21 \times 10^6 \) m/s. Under the matter wave consideration, the particle will behave closely like (h = \( 6.63 \times 10^{-34} \) J.s)