Schulz R J, Venkataramanan N, Huq M S
Department of Therapeutic Radiology, Yale University School of Medicine, New Haven, Connecticut.
Phys Med Biol. 1990 Nov;35(11):1563-74. doi: 10.1088/0031-9155/35/11/010.
The thermal defects of A-150 plastic and graphite referenced to aluminium were determined for 800 keV protons scattered by a 2 micron nickel foil (mean transmitted energy = 550 keV). Composite cores of Al/A-150, graphite/A-150 and Al/graphite which could be irradiated from one side or the other were employed. The temperature increase of a core caused by 30-100 s of irradiation (3-6 nA of proton beam current) was detected by two thermistors mounted in opposite legs of a Wheatstone bridge. The thermal defect of A-150 plastic was determined to be 0.0421 +/- 0.0036 (SE) referenced to aluminium and 0.0402 +/- 0.0034 referenced to graphite. The thermal defect of graphite referenced to aluminium is 0.0043 +/- 0.0034. No change in the thermal defect of A-150 plastic was detected for accumulated doses up to 8 x 10(5) Gy.
针对被2微米镍箔散射的800千电子伏特质子(平均透射能量 = 550千电子伏特),测定了以铝为参考的A - 150塑料和石墨的热缺陷。使用了可以从一侧或另一侧进行辐照的Al/A - 150、石墨/A - 150和Al/石墨复合芯体。通过安装在惠斯通电桥相对臂上的两个热敏电阻检测由30 - 100秒辐照(质子束电流为3 - 6纳安)引起的芯体温度升高。以铝为参考,A - 150塑料的热缺陷被测定为0.0421 ± 0.0036(标准误差),以石墨为参考则为0.0402 ± 0.0034。以铝为参考,石墨的热缺陷为0.0043 ± 0.0034。对于累积剂量高达8×10⁵戈瑞的情况,未检测到A - 150塑料热缺陷的变化。