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Development of an electronic monitor for the determination of individual radon and thoron exposure

机译:开发用于测定单个氡和钍射气暴露的电子监视器

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摘要

The carcinogenic effect of the radio isotope Rn-222 of the noble gas radon and its progeny, as well as its residential distribution, are well studied. In contrast, the knowledge about the effects and average dwelling concentration levels of its radio isotope Rn-220 (thoron) is still limited. Generally, this isotope has been assumed to be a negligible contributor to the effective annual dose. However, only recently it has been pointed out in several international studies, that the dose due to thoron exceeds the one from Rn-222 under certain conditions. Additionally, radon monitors may show a considerable sensitivity towards thoron which was also not accounted for in general. Therefore a reliable, inexpensive exposimeter, which allows to distinguish between decays of either radon and thoron, is required to conduct further studies.udThe scope of this thesis was to develop an electronic radon/thoron exposimeter which features small size, low weight and minimal power consumption. The design is based on the diffusion chamber principle and employs state-of-the-art alpha particle spectroscopy to measure activity concentrations. The device was optimized via inlet layout and filter selection for high thoron diffusion. Calibration measurements showed a similar sensitivity of the monitor towards radon and thoron, with a calibration factor of cfRn-222 = 16.2±0.9 Bq×m-3/cph and cfRn-220 = 14.4±0.8 Bq×m-3/cph, respectively. Thus, the radon sensitivity of the device was enhanced by a factor two compared to a previous prototype. The evaluation method developed in this work, in accordance with ISO 11665 standards, was validated by intercomparison measurements. The detection limits for radon and thoron were determined to be C#Rn-222 = 44.0 Bq/m3 and C#Rn-220 = 40.0 Bq/m3, respectively, in case of a low radon environment, a one-hour measurement interval, and a background count rate of zero. In contrast, in mixed radon/thoron concentrations where the Po-212 peak must be used for thoron concentration determination, a calibration factor of cfRn-220 = 100±10 Bq×m-3/cph was measured, yielding a detection limit of C#Rn-220 = 280 Bq/m3.udFurther, Monte Carlo (MC) simulations were performed by means of various codes including Geant4, to study the effect of the variation of parameters influencing the calibration factors. The results showed reasonable agreement between simulated and acquired spectra, with differences being below 8%, thus validating the employed simulation model. The simulations indicated a significant impact of environmental parameters, such as temperature and pressure, on the measured spectra and accordingly on the calibration factor. Therefore the calibration factor was quantified as a function of temperature, relative humidity and pressure as well as chamber volume. For devices with increased detection volume a considerable influence of air density changes, corresponding to altitudes from 0-5,000 m, and temperatures from -25 to 35 °C, on the calibration factor of up to 32% was observed. In contrast, for devices with standard housing the calibration factor changed only up to 4%. When increasing the detection volume compared to the employed standard housing by at least a factor of four, a maximum increase of the sensitivity of about 20% was found, at the expense of device portability. On the contrary, when reducing the height of the housing by 10~$mm$, which yields 40% less volume, a decrease of sensitivity by 30% and 41% for radon and thoron was observed, respectively.udFinally, devices were used and tested at different realistic conditions, such as mines, radon spas, and dwellings with mixed Rn-222 and Rn-220 environments. Measurements in a salt mine with the device developed within the framework of this thesis revealed maximum radon concentrations of up to 1.0 kBq/m3.udIn the Bad Gastein Heilstollen, Rn-222 concentrations up to 24.3 kBq/m3 were found, in agreement with an AlphaGuard reference device. First measurements in radon/thoron environments of about 200 Bq/m3 each, in a clay model house at the Helmholtz Center Munich, showed reasonable agreement with reference devices, thus validating the introduced evaluation method. First measurements in a private Bavarian clay house revealed a low thoron concentration of about CRn-220 = 13.0±3.0 Bq/m3, in comparison to a high radon concentration of CRn-222 = 200±70 Bq/m3.
机译:稀有气体ra的放射性同位素Rn-222的致癌作用及其子代及其居住分布已得到了很好的研究。相反,关于其放射性同位素Rn-220(220)的影响和平均居住浓度水平的知识仍然有限。通常,该同位素被认为对有效年剂量的贡献可忽略不计。但是,直到最近,在一些国际研究中才指出,在某些条件下,的剂量超过Rn-222的剂量。另外,ra监测器可能显示出对的相当大的敏感性,这在一般情况下也没有考虑。因此,需要可靠,廉价的能区分ra和的衰变的辐射计,以进行进一步的研究。 ud本文的研究范围是开发一种体积小,重量轻,体积小的电子ra / tho电子测光仪。能量消耗。该设计基于扩散室原理,并采用最先进的α粒子光谱技术来测量活性浓度。该设备通过入口布局和过滤器选择进行了优化,以实现高扩散。校准测量结果表明监测仪对ra和具有相似的灵敏度,校准系数分别为cfRn-222 = 16.2±0.9 Bq×m-3 / cph和cfRn-220 = 14.4±0.8 Bq×m-3 / cph 。因此,与先前的原型相比,该装置的ra灵敏度提高了两倍。通过比对测量验证了根据ISO 11665标准在这项工作中开发的评估方法。在低ra环境下,一小时的测量间隔确定ra和的检出限分别为C#Rn-222 = 44.0 Bq / m3和C#Rn-220 = 40.0 Bq / m3。并且背景计数率为零。相反,在必须使用Po-212峰进行气浓度测定的混合// tho气浓度中,测量的校正因子为cfRn-220 = 100±10 Bq×m-3 / cph,检测限为C #Rn-220 = 280 Bq / m3。 ud此外,还通过包括Geant4在内的各种代码进行了蒙特卡洛(MC)仿真,以研究影响校正因子的参数变化的影响。结果表明,模拟光谱和采集光谱之间的合理吻合,差异小于8%,从而验证了所用的模拟模型。模拟表明环境参数(例如温度和压力)对测得的光谱以及因此对校准因子的影响很大。因此,将校准因子量化为温度,相对湿度和压力以及腔室体积的函数。对于具有增加的检测体积的设备,观察到空气密度变化(高达0-5,000 m的高度和-25至35°C的温度)对高达32%的校准系数的影响很大。相反,对于具有标准外壳的设备,校准系数最多只能更改4%。与采用的标准外壳相比,将检测体积增加至少四分之一时,发现灵敏度最大增加了约20%,但以设备的便携性为代价。相反,当将外壳的高度降低10%至$ mm $时,体积减小40%,,和and的灵敏度分别降低30%和41%。 ud最后,使用设备并在不同的实际条件下进行了测试,例如矿山,ra水疗中心以及具有Rn-222和Rn-220混合环境的住宅。在本论文框架内开发的装置中对盐矿进行的测量表明,最高ra浓度可达1.0 kBq / m3。 ud在Bad Gastein Heilstollen中,发现Rn-222浓度高达24.3 kBq / m3,与AlphaGuard参考设备。在慕尼黑Helmholtz中心的粘土模型房屋中,分别在约200 Bq / m3的ra / tho环境中进行的首次测量显示与参考设备合理吻合,从而验证了引入的评估方法。第一次在巴伐利亚私人粘土屋中进行的测量表明,与ron高浓度的CRn-222 = 200±70 Bq / m3相比,离子浓度低,约为CRn-220 = 13.0±3.0 Bq / m3。

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    Irlinger Josef;

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