Anode heel effect

Changed by Joshua Mann, 31 Dec 2017

Updates to Article Attributes

Body was changed:

Anode heel effect refers to the lower field intensity oftowards theanode in comparison to the cathode due to lower x-ray beam, producedemissions from the X-ray tube, which is not uniform in all portions oftarget material at angles perpendicular to the electron beam.

Basic concept

In general,The conversion of the electron beam consistsinto x-rays doesn’t simply occur at the surface of a central raythe 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 a diverging beamfewer are resorbed. The rays

The end result is that the field intensity towards the cathode end ofis more than that towards the tube have more intensity. This is because, in a diverging beamanode. 

Factors

  • anode angle: by increasing the angle, the rays which are parallel or near parallelamount of target material perpendicular to the inclined/angulated anode get absorbed by the anode itself.

    Applications

    1. intensityis decreased resulting in less resorption of beam on the anode side is less than cathode side: therefore place the thicker part of the body on the cathode side, e.g. upper thoracic on the anode side and lower thoracic or upper abdomen should be placed on the cathode sidex-rays produced.
    2. target-to-film distanceincrease in distance reduces heel effect.
    3. size of film (keeping target-to-film distance as constant ): the smaller film has lesser heel effect as the divergent beam does not reach the film and intensity by allowing more divergence of the beam iswhich produces a more uniform image.
    4. field size: the field will be more uniform at the centre than atdue to the peripherycollimator 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
  • -<p><strong>Anode heel effect </strong>refers to the intensity of the x-ray beam, produced from the <a href="/articles/x-ray-tube-1">X-ray tube</a>, which is not uniform in all portions of the beam.</p><h4>Basic concept</h4><p>In general, the beam consists of a central ray and a diverging beam. The rays towards the cathode end of the tube have more intensity. This is because, in a diverging beam, the rays which are parallel or near parallel to the inclined/angulated anode get absorbed by the anode itself.</p><h4>Applications</h4><ol>
  • -<li>intensity of beam on the anode side is less than cathode side: therefore place the thicker part of the body on the cathode side, e.g. upper thoracic on the anode side and lower thoracic or upper abdomen should be placed on the cathode side.</li>
  • -<li>
  • -<strong>target-to-film distance: </strong>increase in distance reduces heel effect.</li>
  • -<li>
  • -<strong>size of film</strong> (keeping target-to-film distance as constant ): the smaller film has lesser heel effect as the divergent beam does not reach the film and intensity of the beam is more uniform at centre than at the periphery.</li>
  • -</ol>
  • +<p><strong>Anode heel effect </strong>refers to the lower field intensity towards the <a href="/articles/anode-1">anode </a>in comparison to the <a href="/articles/cathode-1">cathode </a>due to lower x-ray emissions from the target material at angles perpendicular to the electron beam.</p><h4>Basic concept</h4><p>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.</p><p>The end result is that the field intensity towards the cathode is more than that towards the anode. </p><h4>Factors</h4><ul>
  • +<li>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.</li>
  • +<li>target-to-film distance<strong>: </strong>increase in distance reduces heel effect by allowing more divergence of the beam which produces a more uniform image.</li>
  • +<li>field size: the field will be more uniform at the centre due to the <a href="/articles/beam-collimators">collimator</a> absorbing the peripheral variations.</li>
  • +<li>positioning: by aligning higher attenuating material towards the cathode and lower attenuating material towards the anode the resulting field is more uniform</li>
  • +</ul>

ADVERTISEMENT: Supporters see fewer/no ads

Updating… Please wait.

 Unable to process the form. Check for errors and try again.

 Thank you for updating your details.