when a metallic surface is illuminated with radiation of wavelength λ, the stopping potential is V if the same surface is illuminated with radiation of wavelength 2λ,the stopping potential is V/4.the threshold wavelength for the metallic surface is
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=> 4 λ
Explanation:
Radius in magnetic field of circular orbit,
R = mV / qB = (√2mE) /qB
and Total energy of moving particle in a circular orbit, E = ( q^2 B^2 R^2 ) / 2m
For a Proton enter in a region of magnetic field,
E1 = ( e^2 × B^2 × R^2 ) / 2 × mp _[i]
where M is the mass of proton
Similarly,for a α-particle moves in a uniform magnetic field
E2 =[( 2e )^2 × B^2 × R^2] / 2 × (4mp)
[ ∵ mα = 4mp ] _[ii]
Dividing Eq [ii] by Eq [ii] we get,
E2/E1 = { [ (2e)^2 × B^2 × R^2 / 2 × (4mp) ] × [ 2 × mp / e^2 × B^2 × R^2] }
E2/E1 = 1 => E2 = E1 = 1MeV
The threshold wavelength for the metallic surface is 4 λ !
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