Anode heel effect refers to the lower field intensity towards the anode in comparison to the cathode due to lower x-ray emissions from the target material at angles perpendicular to the electron beam.
The conversion of the electron beam into x-rays doesn’t simply occur at the surface of the target material but deep within it. Because x-rays are produced deep in the target material they must traverse back out of it before they can proceed to the target field. More target material needs to be traversed at emission angles that are perpendicular to the electron beam (closer to the anode) than at those more parallel to it (closer to the cathode). This increase in material leads to more resorption of the x-rays by the target material resulting in fewer x-rays reaching the field at angles perpendicular to the electron beam. It also means that the x-rays emitted to angles closer to the incident beam travel through less target material and fewer are resorbed.
The end result is that the field intensity towards the cathode is more than that towards the anode.
- anode angle: by increasing the angle, the amount of target material perpendicular to the anode is decreased resulting in less resorption of x-rays produced.
- target-to-film distance: increase in distance reduces heel effect by allowing more divergence of the beam which produces a more uniform image.
- field size: the field will be more uniform at the center (i.e. smaller field size) due to the collimator absorbing the peripheral variations.
- positioning: by aligning higher attenuating material towards the cathode and lower attenuating material towards the anode the resulting field is more uniform
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