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QJEEAdv18Phd04f: JEE Advanced 2018 Physics - Class 12 JEEAdv18Phd04f Solution: In a photoelectric experiment a parallel beam of monochromatic…

In a photoelectric experiment a parallel beam of monochromatic light with power of 200200 WW is incident on a perfectly absorbing cathode of work function 6.256.25 ev.ev. The frequency of light is just above the threshold frequency so that the photoelectrons are emitted with negligible kinetic energy. Assume that the photoelectron emission efficiency is 100%100\% . A potential difference of 500500 VV is applied between the cathode and the anode. All the emitted electrons are incident normally on the anode and are absorbed. The anode experiences a force F=n×10−4F = n \times {10^{ - 4}} NN due to the impact of the electrons. The value of nn is ______________. Mass of the electron Me=9×10−31 kg{M_e} = 9 \times {10^{ - 31}}\,kg and 1.0eV=1.6×10−19 J.1.0eV = 1.6 \times {10^{ - 19}}\,J.

Step-by-Step Verified Solution

The frequency of incident light is just above the threshold frequency. Hence, the energy of each photon is equal to the work function (Ep = ϕ\phi = 6.25 eV) and the kinetic energy of emitted photo-electron is zero (Ke0 = 0). The energy incident per second on the cathode is incident power P = 200 W. Thus, number of photons incident per second is

Np = P/Ep = P/ ϕ\phi .

The photo-electron emission efficiency is 100%. Thus, number of photo-electron emitted per second is equal to the number of photons incident per second i.e., Ne = Np. These photo-electrons are accelerated by a potential difference V = 500 V. Thus, gain in potential energy of each photo-electron is Δ\Delta U = eV = 500 eV. By conservation of energy, kinetic energy of the photo-electron when it reaches the anode is

Ke = Ke0 + Δ\Delta U = 500 eV.

The linear momentum of photo-electron of mass me and kinetic energy Ke is given by

pe=2meKe{p_e} = \sqrt {2{m_e}{K_e}} .

The photo-electron transfer its entire linear momentum to the anode (absorbed by the anode). Thus, gain in linear momentum of the anode by absorbing one photo-electron is

Δ\Delta pa = pe.

The force on the anode is equal to the increase in its linear momentum per second. Since Ne photo-electrons strikes the anode per second, the force acting on the anode is given by

Fa=NeΔpa=Nepe{F_a} = {N_e}\Delta {p_a} = {N_e}{p_e} ( ∵\because Δpa=pe\Delta {p_a} = {p_e} )

=Nppe=(P/ϕ)pe= {N_p}{p_e} = (P/\phi ){p_e} ( ∵\because Ne=Np=P/ϕ{N_e} = {N_p} = P/\phi )

=(P/ϕ)2meKe= (P/\phi )\sqrt {2{m_e}{K_e}} ( ∵\because pe=2meKe{p_e} = \sqrt {2{m_e}{K_e}} )

=(P/ϕ)2meeV= (P/\phi )\sqrt {2{m_e}eV} ( ∵\because Ke=eV{K_e} = eV

=2.4×10−4N= 2.4 \times {10^{ - 4}}N .

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