Department of Radiological Sciences, Ibaraki Prefectural University of Health Sciences, 4669-2, Ami-machi, Inashiki-gun, Ibaraki, 300-0394, Japan.
Graduate School of Health Sciences, Department of Radiological Sciences, Ibaraki Prefectural University of Health Sciences, 4669-2, Ami-machi, Inashiki-gun, Ibaraki, 300-0394, Japan.
J Radiat Res. 2020 Sep 8;61(5):712-717. doi: 10.1093/jrr/rraa045.
In this study, we propose a methodology for temperature determination of the temperature and pressure correction factor, PTP, by analyzing the temperature distribution of the modeled ionization chamber taking into account the thermal effect of a water phantom on neighboring materials in the process. Additionally, we present an appropriate temperature-equilibrium time for conducting measurements. The temporal response in the cavity is acquired at 20-s intervals using a Farmer ionization chamber and an electrometer. The initial temperature of the water phantom is 20-25°C with continuous heating/cooling. The temporal response is measured until temperature equilibrium is confirmed, specifically when a temperature difference of 1-5°C is observed between the ionization chamber and the water phantom. Using an ionization-chamber model, temperature distribution is simulated between 20 and 25°C with various parameters set to receive heating and cooling from surrounding media. The results suggest that the temporal response of the ionization chamber essentially coincides with the temperature change at the tip and middle; moreover, the predicted temperature change for temporal response and the simulated temperature of water are different by ~0.16°C at the tip and ~0.79°C at the bottom. Overall, the temperature-equilibration time for absorbed dosimetry is affected by two factors: the cavity wall and the stem side of the cavity; moreover, 400 s is required to obtain complete temperature equilibrium in the water phantom. This analytical study supports the experimental value obtained in previous research. Therefore, analytical representation of the temperature distribution in the ionization chamber is possible.
在这项研究中,我们提出了一种通过分析考虑到水模体对邻近材料的热效应的模型化电离室的温度分布来确定温度和压力校正因子,PTP 的方法。此外,我们还提出了进行测量的适当温度平衡时间。使用 Farmer 电离室和静电计以 20 秒的间隔获取腔内的时间响应。初始水模体温度为 20-25°C,并持续加热/冷却。当在电离室和水模体之间观察到 1-5°C 的温差时,测量时间响应,直到确认温度平衡。使用电离室模型,在 20-25°C 之间模拟各种参数的温度分布,以接收来自周围介质的加热和冷却。结果表明,电离室的时间响应本质上与尖端和中部的温度变化一致;此外,时间响应的预测温度变化和水的模拟温度在尖端相差约 0.16°C,在底部相差约 0.79°C。总体而言,吸收剂量的温度平衡时间受两个因素的影响:腔壁和腔的茎侧;此外,需要 400 秒才能使水模体完全达到温度平衡。这项分析研究支持了先前研究中获得的实验值。因此,电离室中的温度分布可以进行分析表示。