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Question: Electron with de Broglie wavelength \(\lambda\)fall on the target in and X ray tube. The cut off wav...

Electron with de Broglie wavelength λ\lambdafall on the target in and X ray tube. The cut off wavelength (λ0\lambda_{0}) of the emitted X rays is

A

λ0=2mcλ2h\lambda_{0} = \frac{2mc\lambda^{2}}{h}

B

)λ0=2hmc\lambda_{0} = \frac{2h}{mc}

C

)λ0=2m2c2λ2h2\lambda_{0} = \frac{2m^{2}c^{2}\lambda^{2}}{h^{2}}

D

)λ0=λ\lambda_{0} = \lambda

Answer

λ0=2mcλ2h\lambda_{0} = \frac{2mc\lambda^{2}}{h}

Explanation

Solution

: Let K be the kinetic energy of the incident electron.

Its linear momentum, p=2mKp = \sqrt{2mK}

The de Broglie wavelength is related to the linear momentum as

λ=hp=h2mkorK=h22mλ2\lambda = \frac{h}{p} = \frac{h}{\sqrt{2mk}}orK = \frac{h^{2}}{2m\lambda^{2}}

The cut off wavelength of the emitted X rays is related to the kinetic energy of the incident electrons as

hcλ0=K=h22mλ2orλ0=2mcλ2h\frac{hc}{\lambda_{0}} = K = \frac{h^{2}}{2m\lambda^{2}}or\lambda_{0} = \frac{2mc\lambda^{2}}{h}