FKM Kompass
L2

X-rays and their production

X-rays are produced when fast electrons strike a target and either decelerate abruptly, radiating a continuous spectrum of bremsstrahlung, or knock out an inner-shell electron from a target atom, producing sharp characteristic lines whose energies are set by the target element's own atomic energy levels.

Practise this concept

X-rays are commonly produced in an X-ray tube: electrons are accelerated through a large voltage and slammed into a solid metal target. The resulting spectrum of emitted radiation has two distinct components, produced by two different physical mechanisms, and telling them apart is the key to understanding X-ray production.

The first component is a smooth, continuous spectrum called bremsstrahlung, German for "braking radiation." As an incoming electron passes close to a target atom's nucleus, the nucleus's electric field deflects and decelerates it, and an accelerating (or decelerating) charge radiates electromagnetic energy. Because each electron can lose anywhere from a small fraction to almost all of its kinetic energy in a single such deflection, depending on how closely it passes the nucleus, the resulting photon energies span a continuous range up to a sharp maximum set by the electron's full kinetic energy — a photon carrying away all of an electron's energy in one deceleration event sets the shortest possible wavelength in the spectrum.

The second component consists of sharp, narrow peaks called characteristic X-rays, superimposed on the continuous background. These arise from a different process entirely: a sufficiently energetic incoming electron can knock an electron out of an inner shell of a target atom, leaving a vacancy. An electron from a higher shell then drops down to fill that vacancy, emitting a photon whose energy equals the difference between the two atomic energy levels involved — exactly analogous to the discrete-line emission that produces atomic spectra generally, but here the transition is between the innermost, most tightly bound shells. Because these energy-level spacings are set entirely by the target element's own atomic structure, characteristic X-ray line energies are a fingerprint of the target material, independent of the bombarding electrons' exact energy (so long as it exceeds the threshold needed to eject the inner-shell electron in the first place) — this fingerprint is the basis of X-ray fluorescence techniques used to identify unknown materials.

Key ideas

Requires: Quantised energy levels in atoms

Unlocks: Bragg diffraction and crystal structure determination

Common misconceptions

  • X-rays are always produced with a single sharp wavelength, never a continuous spectrum of energies.
  • The characteristic X-ray lines produced by a target depend on the speed of the bombarding electrons rather than on the target material itself.
  • Bremsstrahlung (braking radiation) requires the electron to be completely absorbed by the target, rather than merely decelerated.

Resources

Part of these UT courses

This concept is mapped as covering part of the following course(s) in the University of Tartu curriculum.