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Dual Nature of Radiation and Matter question

2016 · Q135
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Dual Nature of Radiation and Matter question

2016 · Q135

NEETPhysicsDual Nature of Radiation and MatterMCQ+4 / −1
Electrons of mass m with de-Broglie wavelength λ\lambdaλ fall on the target in an X-ray tube. The cutoff wavelength (λ\lambdaλ0) of the emitted X-ray is
  1. A
    λ\lambdaλ0 = 2mcλ2h{{2mc{\lambda ^2}} \over h}h2mcλ2​
  2. B
    λ0=2hmc{\lambda _0} = {{2h} \over {mc}}λ0​=mc2h​
  3. C
    λ0=2m2c2λ3h2{\lambda _0} = {{2{m^2}{c^2}{\lambda ^3}} \over {{h^2}}}λ0​=h22m2c2λ3​
  4. D
    λ0=λ{\lambda _0} = \lambdaλ0​=λ
View written solutionFree

Correct answer: A

Kinetic energy of electrons

K = p22m{{{p^2}} \over {2m}}2mp2​ = (hλ)22m{{{{\left( {{h \over \lambda }} \right)}^2}} \over {2m}}2m(λh​)2​ = h22mλ2{{{h^2}} \over {2m{\lambda ^2}}}2mλ2h2​

For certain frequency, maximum wavelength that can be emitted is λ\lambda λ0 which is cut off wavelength obtained at cut off frequency,

E0 = hcλ0{{hc} \over {{\lambda _0}}}λ0​hc​

Since, E = E0

h22mλ2=hcλ0{{{h^2}} \over {2m{\lambda ^2}}} = {{hc} \over {{\lambda _0}}}2mλ2h2​=λ0​hc​

⇒\Rightarrow⇒ λ\lambda λ0 = 2mcλ2h{{2mc{\lambda ^2}} \over h}h2mcλ2​

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