Question

Difficulty: Very hardX-rays: Production, Properties, and Applications

An X-ray tube operates at an accelerating potential of 50.0 kV50.0\text{ kV}. Given Planck's constant h=6.63×1034 J sh = 6.63 \times 10^{-34}\text{ J s}, the speed of light c=3.00×108 m s1c = 3.00 \times 10^8\text{ m s}^{-1}, and the elementary charge e=1.60×1019 Ce = 1.60 \times 10^{-19}\text{ C}, what is the minimum wavelength λmin\lambda_{\min} of the emitted continuous X-rays, and how does this cutoff wavelength respond to an increase in the anode potential?

  1. 2.49×1011 m2.49 \times 10^{-11}\text{ m}, and λmin\lambda_{\min} decreases when the anode potential is increased.Answer
  2. B
    2.49×108 m2.49 \times 10^{-8}\text{ m}, and λmin\lambda_{\min} decreases when the anode potential is increased.
  3. C
    2.49×1011 m2.49 \times 10^{-11}\text{ m}, and λmin\lambda_{\min} remains unchanged because λmin\lambda_{\min} depends only on the filament current.
  4. D
    4.02×1011 m4.02 \times 10^{-11}\text{ m}, and λmin\lambda_{\min} increases when the anode potential is increased.

Answer

The minimum wavelength is 2.49×1011 m2.49 \times 10^{-11}\text{ m}, and λmin\lambda_{\min} decreases when the anode potential is increased.
By the Duane-Hunt law, the maximum photon energy produced by electron impact equals the kinetic energy of the incident electron: eV=hcλmine V = \frac{h c}{\lambda_{\min}}. Substituting h=6.63×1034 J sh = 6.63 \times 10^{-34}\text{ J s}, c=3.00×108 m s1c = 3.00 \times 10^8\text{ m s}^{-1}, e=1.60×1019 Ce = 1.60 \times 10^{-19}\text{ C}, and V=5.00×104 VV = 5.00 \times 10^4\text{ V} yields λmin=2.49×1011 m\lambda_{\min} = 2.49 \times 10^{-11}\text{ m}. Because λmin\lambda_{\min} is inversely proportional to VV, increasing the anode potential decreases the minimum wavelength, making the beam more penetrating (harder).

Step-by-Step Solution

1
Convert the operating voltage to standard SI units (volts).
V=50.0 kV=50.0×103 V=5.00×104 VV = 50.0\text{ kV} = 50.0 \times 10^3\text{ V} = 5.00 \times 10^4\text{ V}.
Equations involving fundamental constants require input quantities in SI base units.
2
Apply the Duane-Hunt law for maximum photon energy / minimum wavelength in continuous X-ray production.
Emax=eV=hcλmin    λmin=hceVE_{\max} = e V = \frac{h c}{\lambda_{\min}} \implies \lambda_{\min} = \frac{h c}{e V}.
The maximum kinetic energy of an accelerating electron is completely converted into a single photon of minimum wavelength.
3
Substitute the physical values into the minimum wavelength formula.
\(\lambda_{\min} = \frac{(6.63 \times 10^{-34}\text{ J s})(3.00 \times 10^8\text{ m s}^{-1})}{(1.60 \times 10^{-19}\text{ C})(5.00 \times 10^4\text{ V})} = \frac{1.989 \times 10^{-25}}{8.00 \times 10^{-15}} = 2.48625 \times 10^{-11}\text{ m} \approx 2.49 \times 10^{-11}\text{ m}\).
Direct numerical evaluation yields the minimum cutoff wavelength.
4
Analyze the functional relationship between anode potential VV and cutoff wavelength λmin\lambda_{\min}.
Since λmin1V\lambda_{\min} \propto \frac{1}{V}, an increase in VV results in a decrease in λmin\lambda_{\min}.
Higher potential imparts greater kinetic energy to striking electrons, enabling emission of higher-frequency (shorter-wavelength) photons.

Key Concept

Duane-Hunt Law and Control Parameters of X-ray Production
Estimated Time:2m 0s
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