1 土壤介质中氡的运移机制
1.1 射气过程和射气系数
表 1 222Rn在几种介质环境中的反冲射程[5] |
| 介质类型 | 密度/(g·m-3) | 最大射程/nm |
| 空气 | 1.58×10-3 | 53×10-3 |
| 水 | 1.00 | 77 |
| 石英 | 2.65 | 34 |
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南宏杰(1985—), 男, 博士研究生 |
收稿日期: 2024-07-31
网络出版日期: 2025-11-07
基金资助
国家自然科学基金面上项目(12275008)
国家自然科学基金青年科学基金项目(12105363)
版权
222Rn exhalation from soils-Mechanism, measurement and management considerations
Received date: 2024-07-31
Online published: 2025-11-07
Copyright
南宏杰 , 张磊 , 郭秋菊 . 土壤中222Rn的析出:机理、测量及管理建议[J]. 清华大学学报(自然科学版), 2025 , 65(11) : 2334 -2340 . DOI: 10.16511/j.cnki.qhdxxb.2024.27.053
Significance: Radon(222Rn) is a naturally occurring radioactive noble gas. 222Rn is produced from the alpha decay of radium (226Ra), with a relatively long half-life (i.e., 3.8 days). Thus, 222Rn can diffuse and migrate from the rock and soil where it is generated and can enter the air. According to surveys conducted by the World Health Organization, exposure to 222Rn and its short-lived progeny is the second leading cause of lung cancer. The measurement and evaluation of 222Rn release involves not only occupational exposure but also public exposure. Therefore, the measurement of 222Rn exhalation and the dose assessments of 222Rn exposure have always been important concerns in radiation protection. Progress: The entire process of 222Rn moving from the soil to the atmosphere can be divided into three steps: emanation, migration, and exhalation. During the emanation process of 222Rn, 222Rn will obtain a recoil energy of 8.6 × 104 eV from the decay of 226Ra, which will make 222Rn atoms travel through the soil grains at a distance of no more than 50 nm. If produced near the surface of soil grains, 222Rn will leave the grain and stop in the interstitial space (pore), becoming freely movable 222Rn. The fraction of freely movable 222Rn is usually expressed by the emanation coefficient (dimensionless). The emanation coefficient of soil generally ranges from 0.1 to 0.3. In soil with a relatively stable internal environment, the migration of free 222Rn in soil mainly relies on molecular diffusion caused by concentration gradients, eventually entering the atmosphere through the soil-air interface. If only diffusion transport is considered, then Fick's law can be used to describe the migration process of 222Rn and establish a model for 222Rn flux at the soil-air interface. The 222Rn exhalation rate at the soil surface is the 222Rn flux. On-site measurement methods of the soil 222Rn exhalation rate can generally be divided into three categories: accumulation, flow-through, and activated carbon adsorption methods. In actual measurements, different methods can be chosen according to the needs. Conclusions and Prospects: The understanding of the 222Rn diffusion exhalation mechanism and influencing factors is becoming comprehensive, and the measurement methods of the 222Rn exhalation rate for different purposes have been developed. Analyzing the physical processes of 222Rn exhalation from soil and measuring and evaluating the exhalation rate of 222Rn are important for assessing environmental radiation and managing uranium tailings and associated radioactive minerals. Moreover, the exhalation rate of 222Rn is closely related to the radiation environmental safety of on-site supervision of naturally occurring radioactive materials. Because of the complexity and diversity of 222Rn measurement sites, even though the amount of 222Rn release can be measured and calculated relatively accurately, nearly no quantitative deterministic correlation is detected between it and the indoor 222Rn concentration. Thus, the 222Rn exposure dose for key populations is difficult to estimate. The 222Rn exposure dose and health risks for key populations can only be estimated and controlled through measurements of the indoor 222Rn levels. Therefore, although the 222Rn exhalation rate is an important parameter that can be measured and calculated on-site, establishing a fixed exhalation rate limit for regulatory purposes is unsuitable.
Key words: radon; soil; radon exhalation; measurement; management considerations
表 1 222Rn在几种介质环境中的反冲射程[5] |
| 介质类型 | 密度/(g·m-3) | 最大射程/nm |
| 空气 | 1.58×10-3 | 53×10-3 |
| 水 | 1.00 | 77 |
| 石英 | 2.65 | 34 |
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