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JEE Advanced 2000
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Animated Solution for Physics - Atoms and Nuclei: Electrons with energy are incident on the tungsten target of an X-ray tube. K-shell electrons of tungsten have energy. X-rays emitted by the tube contain only

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\text{X-ray Production Mechanisms}

  • \text{Continuous X-rays (Bremsstrahlung): Produced by deceleration of incident electrons.}
  • \text{Characteristic X-rays: Produced when an incident electron knocks out an inner-shell electron.}

\text{Minimum Wavelength of Continuous Spectrum}

  • E_{\text{incident}} = 80 \text{ keV} = 80 \times 10^3 \text{ eV}
  • \lambda_{\text{min}} = \frac{hc}{E_{\text{incident}}}
  • \lambda_{\text{min}} = \frac{12375 \text{ eV \AA}}{80 \times 10^3 \text{ eV}} \approx 0.155 \text{ \AA}

\text{Condition for Characteristic X-rays}

  • \text{Incident energy must be greater than the binding energy of the shell.}
  • E_{\text{incident}} > E_{\text{binding}}

\text{Comparing Energies}

  • E_{\text{incident}} = 80 \text{ keV}
  • E_{\text{K-shell}} = 72.5 \text{ keV}
  • 80 \text{ keV} > 72.5 \text{ keV}

\text{Conclusion}

  • \text{Both continuous and characteristic X-ray spectra are present.}

The Sigma Insight: Bohr's Atomic Model and Energy Levels

Solution Diagram

Analyzing the Setup When high-energy electrons strike a heavy target like tungsten, two distinct types of X-rays are produced

First, we have the continuous X-rays, also known as Bremsstrahlung, which are caused by the rapid deceleration of the incident electrons as they interact with the strong electric fields of the target nuclei. Second, we have the characteristic X-rays, which are emitted when an incident electron successfully knocks out an inner-shell electron (like one from the K-shell), and an outer electron falls in to fill the resulting vacancy.

The Continuous Spectrum Let's first look at the continuous spectrum

The maximum energy an X-ray photon can possess is exactly equal to the total kinetic energy of the incident electron. This maximum energy corresponds to the minimum wavelength, , of the emitted X-rays. Using the standard energy-wavelength relation:
Substituting the given incident energy of (or ) and using for precision, we get:
This confirms that a continuous spectrum with a minimum wavelength of is indeed produced.

The Characteristic Spectrum Now, what about the characteristic X-rays? For these to be emitted, the incident electron must have enough energy to overcome the binding energy of an inner shell and eject an electron

The condition is strictly:
In our problem, the incident electrons have an energy of . The K-shell electrons of tungsten are bound with an energy of . Since , the incident electrons pack enough punch to eject the K-shell electrons!
Because the K-shell vacancy is created, outer shell electrons will drop down to fill it, emitting characteristic X-rays in the process. Therefore, the X-rays emitted by the tube will contain both a continuous spectrum with a minimum wavelength of and the characteristic X-ray spectrum of tungsten.

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