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QJEEAdv16Pha231: JEE Advanced 2016 Physics - Class 12 JEEAdv16Pha231 Solution: Light of wavelength ph falls on a cathode plate inside a vacuum …

Light of wavelength λ\lambda ph falls on a cathode plate inside a vacuum tube as shown in the figure. The work function of the cathode surface is ϕ\phi and the anode is a wire mesh of conducting material kept at a distance d from the cathode. A potential difference V is maintained between the electrodes. If the minimum de-Broglie wavelength of the electrons passing through the anode is λ\lambda e, which of the following statement(s) is (are) true?

JEE Advanced 2016 Paper 2 Offline Physics - Dual Nature of Radiation Question 18 English

Multiple Choice Options

  • A λ\lambda e increases at the same rate as λ\lambda ph for λ\lambda ph < hc/ ϕ\phi
  • B λ\lambda e is approximately halved, if d is doubled
  • C λ\lambda e decreases with increase in ϕ\phi and λ\lambda ph
  • D For large potential difference (V >> ϕ\phi /e), λ\lambda e is approximately halved if V is made four times

Step-by-Step Verified Solution

In photo-electric effect, the maximum kinetic energy of the photo-electron ejected at the cathode, is given by

Kmax⁡, c=hcλph−ϕ{K_{\max ,\,c}} = {{hc} \over {{\lambda _{ph}}}} - \phi ,

where λ\lambda ph is the wavelength of the incident light and ϕ\phi is the work function of the material. The ejected photoelectrons are accelerated from the cathode to the anode by a potential V. Thus, the maximum kinetic energy of the photo-electron at the anode is

Kmax⁡, a=Kmax⁡, c+eV=hcλph−ϕ+eV{K_{\max ,\,a}} = {K_{\max ,\,c}} + eV = {{hc} \over {{\lambda _{ph}}}} - \phi + eV .

Now, minimum de-Broglie wavelength of electrons passing through anode,

λe=h2m Kmax⁡, a=h2m(hcλph−ϕ+eV){\lambda _e} = {h \over {\sqrt {2m\,{K_{\max ,\,a}}} }} = {h \over {\sqrt {2m\left( {{{hc} \over {{\lambda _{ph}}}} - \phi + eV} \right)} }} ...... (i)

D : For V &gt; &gt; \phi e

λe≈h2meV∝1V{\lambda _e} \approx {h \over {\sqrt {2meV} }} \propto {1 \over {\sqrt V }}

∴\therefore If V is made four times, λ\lambda e becomes 14=12{1 \over {\sqrt 4 }} = {1 \over 2} , i.e. halved.

C : When ϕ\phi and λ\lambda ph increases, λ\lambda e also increases.

A : From (i)

dλedt=−h2[2m(hcλph−ϕ+eV)]−3/2×2m(−hcλph2)dλphdt{{d{\lambda _e}} \over {dt}} = {{ - h} \over 2}{\left[ {2m\left( {{{hc} \over {{\lambda _{ph}}}} - \phi + eV} \right)} \right]^{ - 3/2}} \times 2m\left( {{{ - hc} \over {\lambda _{ph}^2}}} \right){{d{\lambda _{ph}}} \over {dt}}

⇒dλedt≠dλphdt\Rightarrow {{d{\lambda _e}} \over {dt}} \ne {{d{\lambda _{ph}}} \over {dt}}

I : λ\lambda e does not depend on d.

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