Wrede D E, Coffey C, Hoskins B, Maruyama Y
Radiol Clin (Basel). 1975;44(6):587-600.
The partial transmission zone (PTZ) measured in air and its radiation shadow components are identified quantitatively and qualitatively for both cuboid and beam-divergence-shaped blocks. Source-block distance (SBD) and source-surface distance (SSD) are varied to produce SBD/SSD ratios from 0.71 to 0.86. The variation of the magnitude of the radiation shadow components as a function of SBD/SSD is explained in terms of a radiation shadow model. The clinical significance of PTZ minimization and a comparison between PTZs of 'shaped' and 'nonshaped' blocks is discussed. For small ratios of SBD/SSD the beam-divergence-shaped blocks produce smaller medial and lateral PTZs, whereas for larger ratios in the order of 0.9 the medial PTZ is also small for the cuboid blocks. Both PTZs, in general, decrease with increasing SBD/SSD ratios and for both cuboid and beam-divergence-shaped blocks.
对长方体和发散束状挡块,定量和定性地识别了在空气中测量的部分透射区(PTZ)及其辐射阴影成分。改变源 - 挡块距离(SBD)和源 - 表面距离(SSD),以产生从0.71到0.86的SBD/SSD比值。根据辐射阴影模型解释了辐射阴影成分大小随SBD/SSD的变化情况。讨论了最小化PTZ的临床意义以及“成形”和“非成形”挡块的PTZ之间的比较。对于较小的SBD/SSD比值,发散束状挡块产生较小的内侧和外侧PTZ,而对于约0.9的较大比值,长方体挡块的内侧PTZ也较小。一般来说,对于长方体和发散束状挡块,两个PTZ都随着SBD/SSD比值的增加而减小。