Cheng Yung Sung, Kenoyer Judson L, Guilmette Raymond A, Parkhurst Mary Ann
Lovelace Respiratory Research Institute, 2425 Ridgecrest Drive SE, Albuquerque, NM 87108, USA.
Health Phys. 2009 Mar;96(3):266-75. doi: 10.1097/01.HP.0000290613.41486.cb.
The Capstone Depleted Uranium (DU) Aerosol Study, which generated and characterized aerosols containing DU from perforation of armored vehicles with large-caliber DU penetrators, incorporated a sampling protocol to evaluate particle size distributions. Aerosol particle size distribution is an important parameter that influences aerosol transport and deposition processes as well as the dosimetry of the inhaled particles. These aerosols were collected on cascade impactor substrates using a pre-established time sequence following the firing event to analyze the uranium concentration and particle size of the aerosols as a function of time. The impactor substrates were analyzed using proportional counting, and the derived uranium content of each served as input to the evaluation of particle size distributions. Activity median aerodynamic diameters (AMADs) of the particle size distributions were evaluated using unimodal and bimodal models. The particle size data from the impactor measurements were quite variable. Most size distributions measured in the test based on activity had bimodal size distributions with a small particle size mode in the range of between 0.2 and 1.2 microm and a large size mode between 2 and 15 microm. In general, the evolution of particle size over time showed an overall decrease of average particle size from AMADs of 5 to 10 microm shortly after perforation to around 1 microm at the end of the 2-h sampling period. The AMADs generally decreased over time because of settling. Additionally, the median diameter of the larger size mode decreased with time. These results were used to estimate the dosimetry of inhaled DU particles.
顶石贫铀(DU)气溶胶研究通过使用大口径贫铀穿甲弹对装甲车辆进行穿孔来生成并表征含贫铀的气溶胶,该研究纳入了一个采样方案以评估粒径分布。气溶胶粒径分布是一个重要参数,它会影响气溶胶的传输和沉积过程以及吸入颗粒的剂量测定。在射击事件发生后,按照预先确定的时间顺序,将这些气溶胶收集在级联撞击器基板上,以分析气溶胶中铀浓度和粒径随时间的变化情况。使用比例计数法对撞击器基板进行分析,每个基板得出的铀含量作为粒径分布评估的输入数据。使用单峰和双峰模型评估粒径分布的活度中值空气动力学直径(AMAD)。撞击器测量得到的粒径数据变化很大。在基于活度的测试中测量的大多数粒径分布具有双峰粒径分布,小粒径模式在0.2至1.2微米范围内,大粒径模式在2至15微米之间。一般来说,粒径随时间的演变表明,穿孔后不久平均粒径从5至10微米的AMAD总体下降,在2小时采样期结束时降至约1微米。由于沉降,AMAD通常随时间减小。此外,较大粒径模式的中值直径也随时间减小。这些结果被用于估计吸入贫铀颗粒的剂量测定。