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Characterization of the energy response and backscatter contribution for two electronic personal dosimeter models

机译:两种电子个人剂量计模型的能量响应和反向散射贡献的表征

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We characterized the energy response of personal dose equivalent ( H p ( 10 ) in mrem) and the contribution of backscatter to the readings of two electronic personal dosimeter (EPD) models with radionuclides commonly used in a nuclear medicine clinic. The EPD models characterized were the RADOS RAD-60R, and the SAIC PD-10i. The experimental setup and calculation of EPD energy response was based on ANSI/HPS N13.11-2009. Fifteen RAD-60R and 2 PD-10i units were irradiated using 99 m Tc , 131 I , and 131 I radionuclides with emission energies at 140 keV, 364 keV, and 511 keV, respectively. At each energy, the EPDs output in H p ( 10 ) [mrem] were recorded with 15 inch thick PMMA to simulate backscatter form the torso. Simultaneous free-in-air exposure rate measurements were also performed using two Victoreen ionization survey meters to calculate the expected EPD H p ( 10 ) values per ANSI/HPS N13.11-2009. The energy response was calculated by taking the ratio of the EPD H p ( 10 ) readings with the expected H p ( 10 ) readings and a two-tailed z -test was used to determine the significance of the ratio deviating away from unity. The contribution from backscatter was calculated by taking the ratio of the EPD H p ( 10 ) readings with and without backscatter material. A paired, two-tailed t -test was used to determine the significance of change in EPD H p ( 10 ) readings. The RAD-60R mean energy response at 140 keV was 0.85, and agreed to within 5% and 11% at 364 and 511 keV, respectively. The PD-10i mean energy response at 140 keV was 1.20, and agreed to within 5% at 364 and 511 keV, respectively. On average, in the presence of acrylic, RAD-60R values increased by 32%, 12%, and 14%, at 140, 364, and 511 keV, respectively; all increases were statistically significant. The PD-10i increased by 25%, 19%, and 10% at 140 keV, 364 keV, and 511 keV, respectively; however, only the 140 keV measurement was statistically significant. Although both EPD models performed within the manufacturers' specifications of ± 25 % in the energy ranges used, they fell outside of our criteria of 10% at lower energies, suggesting the need to calculate energy-dependent correction factors, depending on the intended EPD use.PACS numbers: 87.53.Bn, 87.55.N-, 87.57.U-
机译:我们表征了个人剂量当量的能量响应(以mm表示的H p(10))以及反向散射对两个核医学诊所常用的放射性核素电子剂量计(EPD)模型读数的贡献。 EPD模型的特征是RADOS RAD-60R和SAIC PD-10i。 EPD能量响应的实验设置和计算基于ANSI / HPS N13.11-2009。用发射能量分别为140 keV,364 keV和511 keV的99 m Tc,131 I和131 I放射性核素辐照了15个RAD-60R和2个PD-10i单元。在每种能量下,用15英寸厚的PMMA记录Hp(10)[mrem]中的EPD输出,以模拟躯干的反向散射。还使用两个Victoreen电离测量仪执行了同时在空气中的暴露速率测量,以根据ANSI / HPS N13.11-2009计算预期的EPD H p(10)值。通过将EPD H p(10)读数与预期H p(10)读数的比值计算出能量响应,并使用两尾z检验来确定该比值偏离单位的重要性。通过采用带和不带反向散射材料的EPD H p(10)读数的比率来计算反向散射的贡献。配对的双尾t检验用于确定EPD H p(10)读数变化的重要性。 RAD-60R在140 keV时的平均能量响应为0.85,并且在364和511 keV时分别同意在5%和11%之内。 PD-10i在140 keV时的平均能量响应为1.20,在364和511 keV时分别达到5%以内。平均而言,在丙烯酸存在下,RAD-60R值分别在140、364和511 keV时分别增加了32%,12%和14%。所有增加均具有统计学意义。 PD-10i在140 keV,364 keV和511 keV时分别增加了25%,19%和10%。但是,只有140 keV的测量值具有统计学意义。尽管两种EPD模型在使用的能量范围内均达到制造商规定的±25%的标准,但在较低的能量下它们均超出了我们10%的标准,这表明需要根据预期的EPD用途计算与能量有关的校正系数.PACS编号:87.53.Bn,87.55.N-,87.57.U-

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