Raffaele L, Settineri N, Pergolizzi S, D'Angelo A
IST-Istituto Scientifico per lo studio dei Tumori, Genova.
Radiol Med. 1995 Sep;90(3):304-6.
The wedge factor was experimentally determined as a function of field size and phantom depth for 6-MV X-rays; measurements were performed on a linear accelerator with a motorized wedge filter (universal wedge, nominal wedge angle = 60 degrees). As a result of our experimental work, we can state that: 1) The wedge factor increases linearly with phantom depth (0.275%/cm), almost independent of field size; this change was experimentally related to the beam "hardening" caused by the high Z value of wedge material, as shown by the increase in wedged-field PDD with respect to the corresponding open-field PDD. Neglecting this variation can induce systematic errors in delivered dose, especially when deep-seated tumors are treated with wedge fields. 2) The wedge factor changes, for rectangular fields, according to the "equivalent square law", and not to the dimension in the wedged direction.
通过实验确定了6兆伏X射线的楔形因子与射野大小和模体深度的函数关系;测量是在配备电动楔形滤过器(通用楔形,标称楔形角 = 60度)的直线加速器上进行的。根据我们的实验工作,可以得出以下结论:1)楔形因子随模体深度呈线性增加(0.275%/厘米),几乎与射野大小无关;这种变化在实验上与楔形材料高Z值导致的束流“硬化”有关,如楔形野百分深度剂量相对于相应开野百分深度剂量的增加所示。忽略这种变化会在剂量传递中引起系统误差,特别是在用楔形野治疗深部肿瘤时。2)对于矩形射野,楔形因子根据“等效方定律”变化,而不是根据楔形方向的尺寸变化。