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Charged particle equilibrium corrections for photon sources from 400 keV to 1.4 MeV.

机译:光子源的带电粒子平衡校正为400 keV至1.4 MeV。

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摘要

Lack of charged particle equilibrium (CPE) has practical importance in radiological health protection, in nuclear medicine, and radiobiology where small radioactive point sources irradiate the human body accidentally or may be introduced into the body for diagnostic, therapeutic, or analytical purposes. The absorbed dose under CPE is readily calculated from knowledge of the photon energy fluence and mass-absorption coefficient of the material. When estimating absorbed dose rates at points close to the source, the primary radiation field varies appreciably over the region within the range of secondary particles. Under such conditions, CPE does not exist and prediction of absorbed dose becomes difficult. However, if one applies correction factors for non-CPE conditions, absorbed dose rates can be calculated fairly easily. In this dissertation, a CPE model was developed for non-CPE conditions to predict the fraction of charged particle equilibrium (ΓCPE) attained in a water medium for point sources of energies in the range from 400 keV to 1.4 MeV using EGS4-DOSRZ Monte Carlo calculation. A new methodology to calculate absorbed dose and kerma along the central axis of the cylindrical phantom was presented and the results were found to be in excellent agreement with published values. In order to corroborate with the EGS4-DOSRZ calculation, another model based on the Klein-Nishina single scattering cross section was developed to quantify the ΓCPE attained in water for point sources. A CPE path length coefficient (μ cm−1) was found for each photon energy and compared with published values. This coefficient was used to determine dose rates averaged over 1 cm2 at depths that are of interest in skin dose exposures. Experimental measurements of CPE were carried out for a Co-60 point source using GAFCHROMIC® MD-55 film (1990) as the dosimetry media. The films were read using a document scanner. Dose rates obtained using the scanner method were compared with those obtained using the single scattering model and excellent agreement was observed. Finally, the empirical model for ΓCPE was implemented in a point kernel dose calculation code WISE and SIMPLE. A Windows-based user interface was also created for the modified code. The code was tested for various geometries and the results compared against those obtained using a very popular commercial code, MICROSHIELD©.
机译:缺乏带电粒子平衡(CPE)在放射健康保护,核医学和放射生物学中具有重要的现实意义,在这些领域中,小的放射性点源会意外照射人体或可能出于诊断,治疗或分析目的而引入人体。根据对材料的光子能量通量和质量吸收系数的了解,可以很容易地计算出CPE下的吸收剂量。在估算接近源的点处的吸收剂量率时,一次辐射场在二次粒子范围内的整个区域内会发生明显变化。在这样的条件下,不存在CPE,并且吸收剂量的预测变得困难。但是,如果对非CPE条件应用校正因子,则可以相当容易地计算吸收剂量率。本文针对非CPE条件建立了CPE模型,用于预测水介质中点能量在400 keV至300 keV之间的带电粒子平衡分数(Γ CPE )。使用EGS4-DOSRZ蒙特卡罗计算得出1.4 MeV。提出了一种新的方法来计算沿圆柱体模中心轴的吸收剂量和比释动能,结果与已发表的值非常吻合。为了证实EGS4-DOSRZ的计算,开发了另一个基于Klein-Nishina单散射横截面的模型来量化点源在水中获得的ΓCPE。发现每个光子能量的CPE路径长度系数(μcm -1 ),并将其与公开的值进行比较。该系数用于确定皮肤剂量暴露感兴趣深度处平均1 cm 2 的剂量率。使用GAFCHROMIC®super-MD-55胶片(1990)作为剂量测定介质,对Co-60点源进行了CPE的实验测量。使用文件扫描仪读取胶片。将使用扫描仪方法获得的剂量率与使用单一散射模型获得的剂量率进行比较,观察到了极好的一致性。最后,在点核剂量计算代码WISE和SIMPLE中实现了Γ CPE 的经验模型。还为修改后的代码创建了一个基于Windows的用户界面。测试了该代码的各种几何形状,并将结果与​​使用非常流行的商业代码MICROSHIELD ©所获得的结果进行了比较。

著录项

  • 作者

    Vasudevan, Latha.;

  • 作者单位

    Texas A&M University.;

  • 授予单位 Texas A&M University.;
  • 学科 Engineering Nuclear.
  • 学位 Ph.D.
  • 年度 2002
  • 页码 140 p.
  • 总页数 140
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类 原子能技术;
  • 关键词

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