To solve this problem, we need to understand the relationship between the wavelengths of the incident electromagnetic wave and the de-Broglie wavelength of the emitted photoelectron. The problem involves Photoelectric Effect and de-Broglie Hypothesis.
Conceptual Understanding:
- The Photoelectric Effect explains that when light of sufficient frequency (or energy) strikes a material, it emits electrons. The energy of the incident photon should be sufficient to overcome the work function of the material.
- The de-Broglie Hypothesis states that every moving particle or object has an associated wave. For a particle like an electron, the de-Broglie wavelength \( \lambda_d \) is given by: \(\lambda_d = \frac{h}{p}\), where \( p \) is the momentum of the particle.
Solution Steps and Equations:
- The energy of the incident photon with wavelength \( \lambda \) is given by: \(E = \frac{hc}{\lambda}\), where \( h \) is Planck's constant and \( c \) is the speed of light.
- As the work function is negligible, all the energy of the photon goes into the kinetic energy of the emitted electron. Thus, the kinetic energy \( K \) is: \(K = \frac{hc}{\lambda}\).
- The kinetic energy is also related to the de-Broglie wavelength by the relation: \(K = \frac{p^2}{2m}\), where \( p \) is the momentum and \( m \) is the mass of the electron.
- From the de-Broglie relation \(\lambda_d = \frac{h}{p}\), we can express the momentum as: \(p = \frac{h}{\lambda_d}\).
- Substitute for \( p \) in the kinetic energy relation: \(K = \frac{\left(\frac{h}{\lambda_d}\right)^2}{2m} = \frac{h^2}{2m\lambda_d^2}\).
- Equating the two expressions for kinetic energy: \(\frac{hc}{\lambda} = \frac{h^2}{2m\lambda_d^2}\).
- Solving for \( \lambda \): \(\lambda = \frac{2mc}{h} \lambda_d^2\).
Thus, the correct relation consistent with the de-Broglie hypothesis and the photoelectric effect is: \(\lambda=(\frac{2mc}{h})\lambda d^2\).
Conclusion: This equation correctly relates the wavelength of the incident electromagnetic wave, the de-Broglie wavelength, and other constants. Thus, the correct answer is option: \(\lambda=(\frac{2mc}{h})\lambda d^2\).