Technical note: Water‐equivalent thickness of Superflab bolus material at diagnostic x‐ray energies
Purpose The purpose of this work was to determine the water‐equivalent thickness of Superflab bolus material for narrow and broad field‐of‐view (FOV) x‐ray geometries at diagnostic x‐ray energies. Methods Transmission measurements were performed for incremental thicknesses of Superflab bolus materia...
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Veröffentlicht in: | Medical physics (Lancaster) 2023-02, Vol.50 (2), p.1237-1241 |
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Sprache: | eng |
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Zusammenfassung: | Purpose
The purpose of this work was to determine the water‐equivalent thickness of Superflab bolus material for narrow and broad field‐of‐view (FOV) x‐ray geometries at diagnostic x‐ray energies.
Methods
Transmission measurements were performed for incremental thicknesses of Superflab bolus material and water in narrow and broad FOV x‐ray geometries. The transmission data was fit to a non‐linear model for x‐ray transmission ‐ the Archer model. Water‐equivalent thickness of Superflab was calculated based upon fitting parameters to transmission curves for 75, 95, and 115 kV x‐ray tube voltages. Measured x‐ray transmission factors for water and Superflab were used to determine the water equivalence of Superflab.
Results
For all x‐ray tube voltages and geometries, the water equivalence of Superflab was greater than one, indicating that Superflab is more attenuating than water. This effect was stronger for broad FOV geometries. At 95 kV, 30 cm of Superflab corresponded to 32.0 cm of water in the narrow FOV geometry, and 34.3 cm of water in the broad FOV geometry. The Archer model fitting parameters and Superflab water equivalence are reported for all x‐ray beam conditions explored in this work.
Conclusions
Superflab bolus material is more attenuating than water at diagnostic x‐ray energies. The Archer model and its respective fitting parameters reported in this work may be used to estimate the water‐equivalent thickness of Superflab for diagnostic x‐ray spectra. |
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ISSN: | 0094-2405 2473-4209 |
DOI: | 10.1002/mp.16147 |