An electromagnetic wave of wavelength ‘λ’ is incident on a photosensitive surface of negligible work function. If ‘m’ mass is of photoelectron emitted from the surface has de-Broglie wavelength λd, then :

  1. \(\lambda = \left( {\frac{{2h}}{{mc}}} \right)\lambda {d^2}\)
  2. \(\lambda = \left( {\frac{{2m}}{{hc}}} \right)\lambda {d^2}\)
  3. \({\lambda _d} = \left( {\frac{{2mc}}{h}} \right){\lambda ^2}\)
  4. \(\lambda = \left( {\frac{{2mc}}{h}} \right){\lambda _d}^2\)

Answer (Detailed Solution Below)

Option 4 : \(\lambda = \left( {\frac{{2mc}}{h}} \right){\lambda _d}^2\)
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Detailed Solution

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Concept:

Photosensitive material are materials which eject electrons when photon of frequency greater than their threshold frequency is incident on the surface.

Einstein's photoelectric equation

\(\frac{{hc}}{\lambda }={ϕ _0} + k\)

ϕ: work function

k = maximum kinetic energy of photoelectrons

Calculation:

As per Einstein's photoelectric equation

\(\frac{{hc}}{\lambda }={ϕ _0} + k\)

ϕ: work function

k = maximum kinetic energy of photoelectrons

As per question, ϕ → 0

\(\therefore = \frac{{hc}}{\lambda } = k = \frac{{{P^2}}}{{2m}} \Rightarrow P = \sqrt {\frac{{2mhc}}{\lambda }} \)

Now De-broglie wavelength

\({\lambda _d} = \frac{h}{P} = \frac{h}{{\sqrt {2mhc/\lambda } }}\)

\( \Rightarrow \sqrt \lambda = {\lambda _d}\sqrt {\frac{{2mc}}{h}} \)

\( \Rightarrow \lambda = \left( {\frac{{2mc}}{h}} \right)\lambda _d^2\)

Hence Option 4) is correct choice.

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