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, λmin, of the emitted X-rays. Using the standard energy-wavelength relation:
Substituting the given incident energy of 80 keV (or 80×103 eV) and using hc≈12375 eV A˚ for precision, we get:
λmin=80×10312375≈0.155 A˚
This confirms that a continuous spectrum with a minimum wavelength of ≈0.155 A˚ 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 80 keV. The K-shell electrons of tungsten are bound with an energy of 72.5 keV. Since 80 keV>72.5 keV, 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 ≈0.155 A˚ and the characteristic X-ray spectrum of tungsten.