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首页> 外文期刊>Romanian reports in physics >NEW DATA CONCERNING THE EFFICIENCY CALIBRATION OF A DRUM WASTE ASSAY SYSTEM. PART I: EXPERIMENTAL CALIBRATION
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NEW DATA CONCERNING THE EFFICIENCY CALIBRATION OF A DRUM WASTE ASSAY SYSTEM. PART I: EXPERIMENTAL CALIBRATION

机译:有关桶废物评估系统效率校准的新数据。第一部分:实验校准

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The study is focused on the efficiency calibration of the gamma spectroscopy system used in the NIPNE drum waste assay facility. The measurement of a radioactive drum waste is generally difficult because of its high volume, the complex and usually unknown distribution of the waste in the drum and its high self-attenuation. To solve these problems, a complex calibration of the system is required. For this purpose, a calibration drum filled with Portland cement and provided with seven tubes, placed at different distances from its center was used. For the efficiency calibration appropriate for a uniformly distributed source, the shell method, using a linear source of ~(152)Eu, was applied. The linear calibration source was introduced successively in the seven tubes, the gamma-spectra were collected while the drum was translated and simultaneously rotated. Using the GENIE-PC software, the gamma-spectra were analyzed and the detection efficiencies were obtained. For the efficiency calibration in the case of a non-homogeneous source, supplemental measurements in the following geometries were made. First with a point source of ~(152)Eu placed in front of the detector, measured in all seven tubes, the dram being only rotated. Second with the linear source of ~(152)Eu placed in front of the detector, measured in all seven tubes, the drum being only rotated. For each case the gamma spectra were recorded and the detection efficiency was calculated.
机译:该研究的重点是NIPNE鼓式废物分析设备中使用的伽马光谱系统的效率校准。由于放射性废物桶的体积大,废物在废物桶中的分布复杂且通常未知,并且其自衰减高,因此通常很难测量放射性废物桶。为了解决这些问题,需要对系统进行复杂的校准。为此,使用了一个装有波特兰水泥并装有七个管的校准鼓,该校准鼓与中心的距离不同。对于适用于均匀分布源的效率校准,应用了使用〜(152)Eu线性源的壳法。将线性校准源依次引入到七个试管中,同时平移和旋转感光鼓,同时收集伽玛光谱。使用GENIE-PC软件分析了伽玛光谱,并获得了检测效率。为了在非均匀源的情况下进行效率校准,在以下几何形状中进行了补充测量。首先,在检测器的前面放置一个〜(152)Eu的点源,在所有七个试管中进行测量,仅旋转感光鼓。其次,将线性(〜152Eu)源放置在检测器前面,在所有七个管中进行测量,仅旋转感光鼓。对于每种情况,记录伽玛光谱并计算检测效率。

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