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通过贝塔活度测量计算顶点贫铀气溶胶浓度。

Calculating Capstone depleted uranium aerosol concentrations from beta activity measurements.

作者信息

Szrom Frances, Falo Gerald A, Parkhurst Mary Ann, Whicker Jeffrey J, Alberth David P

机构信息

U.S. Army Center for Health Promotion and Preventive Medicine, 5158 Blackhawk Road, Aberdeen Proving Ground, MD 21010-5403, USA.

出版信息

Health Phys. 2009 Mar;96(3):238-50. doi: 10.1097/01.HP.0000290612.27848.cd.

Abstract

Beta activity measurements were used as surrogate measurements of uranium mass in aerosol samples collected during the field testing phase of the Capstone Depleted Uranium (DU) Aerosol Study. These aerosol samples generated by the perforation of armored combat vehicles were used to characterize the DU source term for the subsequent Human Health Risk Assessment (HHRA) of Capstone aerosols. Establishing a calibration curve between beta activity measurements and uranium mass measurements is straightforward if the uranium isotopes are in equilibrium with their immediate short-lived, beta-emitting progeny. For DU samples collected during the Capstone study, it was determined that the equilibrium between the uranium isotopes and their immediate short-lived, beta-emitting progeny had been disrupted when penetrators had perforated target vehicles. Adjustments were made to account for the disrupted equilibrium and for wall losses in the aerosol samplers. Values for the equilibrium fraction ranged from 0.16 to 1, and the wall loss correction factors ranged from 1 to 1.92. This paper describes the process used and adjustments necessary to calculate uranium mass from proportional counting measurements.

摘要

在“顶点”贫铀(DU)气溶胶研究的现场测试阶段,β活度测量被用作所采集气溶胶样品中铀质量的替代测量方法。这些由装甲战车穿孔产生的气溶胶样品用于确定“顶点”气溶胶后续人类健康风险评估(HHRA)的DU源项。如果铀同位素与其直接的短寿命β发射子体处于平衡状态,那么在β活度测量和铀质量测量之间建立校准曲线很简单。对于在“顶点”研究期间采集的DU样品,已确定当侵彻体穿透目标车辆时,铀同位素与其直接的短寿命β发射子体之间的平衡被打破。进行了调整以考虑被打破的平衡以及气溶胶采样器中的壁损失。平衡分数值范围为0.16至1,壁损失校正因子范围为1至1.92。本文描述了从比例计数测量计算铀质量所使用的过程和必要的调整。

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