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A Compensator for Variations in Tissue Thickness for High Energy Beams
113
Citations
3
References
1959
Year
Tissue EngineeringHigh Energy BeamsEngineeringMechanical EngineeringTissue ThicknessRadiation ExposureBiomedical EngineeringOrthopaedic SurgeryRadiation ProtectionBeam OpticMechanicsBiomechanicsKv X-ray TherapyWax BlockRadiation Therapy PlanningRadiation OncologyNuclear MedicineCollimationRadiologyHealth SciencesMechanobiologyCobalt 60Medical ImagingRadiation ApplicationRadiation EffectsDosimetryBeam Transport System
High‑energy radiation beams spare the skin due to dose build‑up below the surface, but using a wax platform to flatten patient contours, as in 250 kV X‑ray therapy, compromises this advantage at higher energies. The authors devised a method to preserve skin sparing while maintaining dose accuracy with high‑energy beams. By moving the wax block away from the skin so secondary electrons cannot reach it and reducing its lateral dimensions to match the increased source distance, the method keeps skin sparing and dose absorption unchanged. Physical measurements showed that omitting the absorber caused 10–30 % deviations from standard isodose curves. See reference 1.
When high energy radiation beams are used, it is an important fact that the skin may be spared to some extent, since the dose builds up to a maximum at a depth below the surface. When we started to use a cobalt 60 beam unit, it was obvious that the technique used by us in 250 kV X-ray therapy, of building a wax platform to convert the irregular contours of a patient into a flat surface, is undesirable at higher energies, because it sacrifices the skin-sparing advantage of the build-up. Physical measurements showed that the absence of an absorber resulted in deviations from standard isodose curves of the order of 10 to 30 per cent. The following method was devised by one of us (FE) to overcome this difficulty. If, instead of being in contact with the skin, the wax block is displaced away from the skin to a distance sufficient to ensure that secondary electrons from the wax do not reach the skin, the skin-sparing effect is preserved. At the same time, the absorption along any given ray is independent of whether the wax is in contact with the skin or displaced from it, provided that the lateral dimensions of the wax block at right angles to the beam direction are reduced to allow for its change of distance from the source, while its thickness remains unaltered (Fig. 1).
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