Department of Radiation Physics, and Department of Medical and Health Sciences, Linköping University, 58183 Linköping, Sweden.
Health Phys. 2020 Sep;119(3):327-341. doi: 10.1097/HP.0000000000001254.
Inhalation of uranium aerosols is a concern in nuclear fuel fabrication. Determination of committed effective doses and lung equivalent doses following inhalation intake requires knowledge about aerosol characteristics; e.g., the activity median aerodynamic diameter (AMAD). Cascade impactor sampling of uranium aerosols in the breathing zone of nuclear operators was carried out at a nuclear fuel fabrication plant producing uranium dioxide via ammonium uranyl carbonate. Complementary static sampling was carried out at key process steps. Uranium on impaction substrates was measured using gross alpha counting and alpha spectrometry. Activity size distributions were evaluated for both unimodal and bimodal distributions. When a unimodal distribution was assumed, the average AMAD in the operator breathing zone at the workshops was 12.9-19.3 μm, which is larger than found in previous studies. Certain sampling occasions showed variable isotope ratios (U/U) at different impactor stages, indicating more than one population of particles; i.e., a multimodal activity size distribution. When a bimodal distribution (coarse and fine fraction) was assumed, 75-88% of the activity was associated with an AMAD of 15.2-18.9 μm (coarse fraction). Quantification of the AMAD of the fine fraction was associated with large uncertainties. Values of 1.7-7.1 μm were obtained. Static sampling at key process steps in the workshops showed AMADs of 4.9-17.2 μm, generally lower than obtained by breathing zone sampling, when a unimodal distribution was assumed. When a bimodal distribution was assumed, a smaller fraction of the activity was associated with the coarse fraction compared to breathing zone sampling. This might be due to impactor positioning during sampling and sedimentation of large particles. The average committed effective dose coefficient for breathing zone sampling and a bimodal distribution was 1.6-2.6 μSv Bq for U when Type M/S absorption parameters were assumed (5.0 μSv Bq for an AMAD of 5 μm). The corresponding lung equivalent dose coefficient was 3.6-10.7 μSv Bq (29.9 μSv Bq for an AMAD of 5 μm). The predicted urinary excretion level 100 d after inhalation intake was found to be 13-34% of that corresponding to an AMAD of 5 μm. Uranium aerosols generated at a nuclear fuel fabrication plant using ammonium uranyl carbonate route of conversion were associated with larger AMADs compared to previous work, especially when sampling of aerosols was carried out in the operator breathing zone. A bimodal activity size distribution can be used in calculations of committed effective doses and lung equivalent doses, but parameters associated with the fine fraction must be interpreted with care due to large uncertainties.
吸入铀气溶胶是核燃料制造过程中的一个关注点。要确定吸入摄入后累积有效剂量和肺当量剂量,需要了解气溶胶特性;例如,空气动力学直径中值(AMAD)。在生产二氧化铀的核燃料制造工厂中,对核操作人员呼吸区的铀气溶胶进行了级联撞击器采样,采用静态采样对关键工艺步骤进行了补充。使用总α计数和α能谱法测量撞击基板上的铀。对单峰和双峰分布进行了活性粒度分布评估。当假设为单峰分布时,车间操作人员呼吸区的平均 AMAD 为 12.9-19.3 μm,大于以往研究结果。在某些采样情况下,不同撞击器阶段的同位素比值(U/U)不同,表明存在不止一种颗粒群;即多峰活性粒度分布。当假设双峰分布(粗粒和细粒)时,75-88%的活性与 AMAD 为 15.2-18.9 μm(粗粒)相关。细粒部分 AMAD 的定量存在较大的不确定性。获得的数值为 1.7-7.1 μm。当假设单峰分布时,车间关键工艺步骤的静态采样得到的 AMAD 为 4.9-17.2 μm,通常低于呼吸区采样结果。当假设双峰分布时,与呼吸区采样相比,活性的较小部分与粗粒部分相关。这可能是由于采样过程中撞击器的定位以及大颗粒的沉降所致。当假设呼吸区采样和双峰分布,且吸收参数为 M/S 型时,1.6-2.6 μSv Bq 为 U 的平均累积有效剂量系数(5 μm 时为 5.0 μSv Bq)。相应的肺当量剂量系数为 3.6-10.7 μSv Bq(5 μm 时为 29.9 μSv Bq)。吸入摄入 100 天后预测的尿液排泄水平为 13-34%,与 5 μm AMAD 相对应。与之前的工作相比,使用碳酸双氧铀路线转化的核燃料制造厂产生的铀气溶胶的 AMAD 较大,特别是在操作人员呼吸区进行气溶胶采样时。双峰活性粒度分布可用于计算累积有效剂量和肺当量剂量,但由于存在较大的不确定性,必须谨慎解释与细颗粒相关的参数。