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The effect of high dose rate on tissue equivalent proportional counter measurements in mixed neutron-gamma fields.

机译:高剂量率对混合中子-伽马场中组织当量比例计数器测量的影响。

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摘要

Tissue equivalent proportional counters (TEPCs) are commonly used for radiation monitoring in areas where a mixture of neutron and photon radiations may be present, such as those commonly encountered in nuclear power plants. In such radiation fields, the dose rate of each component can vary drastically from extremely low to very high. Among these possible combinations of radiation fields with very different dose rates, a mixed field of an intense photon and a weak neutron dose component is the more commonly encountered.;We have observed that high dose rates due to both photons and neutrons in a mixed field of radiation result in pile up of pulses and distort the lineal energy spectrum measured under these conditions. The pile up effect and hence the distortion in the lineal energy spectrum becomes prominent with dose rates which result in dead times larger than 25% for the high LET radiation component. In intense neutron fields, which may amount to 75% dead time, a 50% or even larger increase in values for the measured microsdosimetric averages and the neutron quality factor was observed. This study demonstrates that moderate dose rates which do not result in dead times of more than 20--25% due to either of the component radiations or due to both components of mixed field radiation generate results which are acceptable for operational health physics mixed neutron-gamma radiation monitoring using tissue equivalent proportional counters.;This study describes the measurement of lineal energy spectra carried out with a 5.1 cm (2 inch) diameter spherical TEPC simulating a 2 microm diameter tissue site in low energy (33--330 keV neutrons) mixed photon-neutron fields with varying dose rates generated by the McMaster University 1.25 MV double stage Tandetron accelerator. The Tandetron accelerator facility was employed to produce neutrons using thick 7Li targets via the 7Li(p, n)7Be reaction. A continuous spectrum of neutrons is generated at any selected proton beam energy which is very narrow at beam energies very close to the threshold of the reaction 1.88 MeV and becomes wider as the proton beam energy moves further away from the threshold energy of the reaction. Dose rates which resulted in dead times as high as 75% for the data acquisition system were employed to study the effect of dose rate on the measured quality factors, microdosimetric averages (y¯f and y¯D) absorbed dose and dose equivalent. The dose rate at a given beam energy was varied by changing the accelerator beam current. A variety of mixed neutron gamma fields was generated using neutron beams with mean energies extending approximately from 33 keV to 330 keV with the 7Li target using proton beam energies ranging from 1.89 to 2.5 MeV. In direct beams, 478 keV photons which are produced in the 7Li target via inelastic scattering interaction 7Li(p, p'gamma) 7Li dominate the low LET component of the mixed field of radiation. When a 2 cm thick polyethylene moderator was inserted between the neutron producing target and the counter, the low LET component of the mixed radiation field also contained 2.20 MeV gamma rays originating from 1H( n, gamma)2H capture interactions in the moderator.
机译:组织等效比例计数器(TEPC)通常用于可能存在中子和光子辐射混合的区域(例如核电站中经常遇到的区域)中的辐射监视。在这样的辐射场中,每种成分的剂量率可以从极低到极高变化很大。在具有不同剂量率的辐射场的这些可能组合中,更常见的是强光子和弱中子剂量成分的混合场。;我们已经观察到,由于光子和中子在混合场中都具有高剂量率辐射的辐射会导致脉冲堆积,并扭曲在这些条件下测得的线性能谱。随着剂量率的增加,堆积效应以及由此线性能谱的畸变变得显着,这导致高LET辐射分量的死区时间大于25%。在强中子场中(可能达到75%的停滞时间),观察到的测得的微剂量平均值和中子品质因数的值增加了50%甚至更大。这项研究表明,适度的剂量率不会由于组分辐射或混合场辐射的两个组分而导致死区时间超过20--25%,产生的结果对于操作健康物理学混合中子-可接受。使用组织等效比例计数器进行伽马辐射监测;这项研究描述了使用线径为5.1厘米(2英寸)的球形TEPC在低能(33--330 keV中子)中模拟直径为2微米的组织部位进行的线性能谱的测量由麦克马斯特大学1.25 MV双级Tandetron加速器产生的具有不同剂量率的混合光子中子场。 Tandetron加速器设备用于通过7Li(p,n)7Be反应使用厚的7Li靶产生中子。在任何选定的质子束能量下都会产生连续的中子光谱,该质子束能量在非常接近反应阈值1.88 MeV的束能量处非常窄,并且随着质子束能量进一步远离反应的阈值能量而变宽。剂量率导致数据采集系统的死区时间高达75%,用于研究剂量率对测得的质量因子,微剂量平均(yf和yd)吸收剂量和剂量当量的影响。通过改变加速器束电流,可以改变给定束能量下的剂量率。使用中子束产生了多种混合中子伽马场,中子束的平均能量范围从33 keV到330 keV,7Li靶标的质子束能量在1.89到2.5 MeV之间。在直射光束中,通过非弹性散射相互作用在7Li目标中产生的478 keV光子7Li(p,p'γ)7Li主导了辐射混合场的低LET分量。当在中子产生靶和计数器之间插入2 cm厚的聚乙烯减速剂时,混合辐射场的低LET分量也包含2.20 MeV伽马射线,该射线源于减速剂中的1H(n,γ)2H捕获相互作用。

著录项

  • 作者

    Qashua, Nael.;

  • 作者单位

    University of Ontario Institute of Technology (Canada).;

  • 授予单位 University of Ontario Institute of Technology (Canada).;
  • 学科 Engineering Nuclear.
  • 学位 M.A.Sc.
  • 年度 2010
  • 页码 87 p.
  • 总页数 87
  • 原文格式 PDF
  • 正文语种 eng
  • 中图分类
  • 关键词

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