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Cut-off Wavelength of X-rays from Incident Electrons

Electrons with de-Broglie wavelength λ\lambda fall on the target in an X-ray tube. The cut-off wavelength of the emitted X-rays is

Options

A

λ0=2mcλ2h\lambda_0 = \frac{2mc\lambda^2}{h}

Correct
B

λ0=2hmc\lambda_0 = \frac{2h}{mc}

C

λ0=2m2c2λ3h2\lambda_0 = \frac{2m^2 c^2 \lambda^3}{h^2}

D

λ0=λ\lambda_0 = \lambda

Step-by-Step Solution

To find the cut-off wavelength (λ0\lambda_0) of the emitted X-rays, we relate the kinetic energy of the incident electrons to the maximum energy of the emitted photons.

  1. Kinetic Energy of the Electron:
    The de-Broglie wavelength λ\lambda of an electron of mass mm and momentum pp is given by:
    λ=hp  ⟹  p=hλ\lambda = \frac{h}{p} \implies p = \frac{h}{\lambda}

The kinetic energy KK of the electron is given by:
K=p22m=h22mλ2K = \frac{p^2}{2m} = \frac{h^2}{2m\lambda^2}

  1. Cut-off Wavelength of the Emitted X-rays:
    In an X-ray tube, the minimum (cut-off) wavelength λ0\lambda_0 corresponds to the maximum photon energy, which occurs when the entire kinetic energy of the incident electron is converted into a single X-ray photon:
    Emax=KE_{\text{max}} = K
    hcλ0=h22mλ2\frac{hc}{\lambda_0} = \frac{h^2}{2m\lambda^2}

  2. Solving for λ0\lambda_0:
    cλ0=h2mλ2\frac{c}{\lambda_0} = \frac{h}{2m\lambda^2}
    λ0=2mcλ2h\lambda_0 = \frac{2mc\lambda^2}{h}

Therefore, the correct option is (A).