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在聚酯树脂体模中确定管电压变化时的计算机断层扫描剂量指数。

Identification of the computed tomography dose index for tube voltage variations in a polyester-resin phantom.

作者信息

Fatichah Lintang N, Anam Choirul, Sutanto Heri, Naufal Ariij, Rukmana Dito A, Dougherty Geoff

机构信息

Department of Physics, Faculty of Sciences and Mathematics, Diponegoro University, Jl. Prof Soedarto SH, Tembalang, Semarang, 50275, Central Java, Indonesia.

Department of Physics, Faculty of Sciences and Mathematics, Diponegoro University, Jl. Prof Soedarto SH, Tembalang, Semarang, 50275, Central Java, Indonesia.

出版信息

Appl Radiat Isot. 2023 Feb;192:110605. doi: 10.1016/j.apradiso.2022.110605. Epub 2022 Dec 5.

Abstract

The aim of this study is to measure the volumetric computed tomography dose index (CTDI) for different tube voltages for a polyester-resin (PESR) phantom, and to compare it to values for a standard polymethyl methacrylate (PMMA) phantom. Both phantoms are head phantoms with a diameter of 16 cm. The phantoms were scanned by a CT scanner (GE Revolution EVO 64/128 slice) with tube voltages of 80, 100, 120, and 140 kV. The other scan parameters were constant (i.e. tube current of 100 mA, rotation time of 1 s, and collimation width of 10 mm). The CTDI and CTDI were obtained by measuring the dose with an ionization chamber inserted into five holes within the phantoms. The CTDI was calculated based on the CTDI and CTDI values. The measurements were repeated three times for each hole. It was found that the CTDI values for the PESR phantom were dependent on tube voltage value, and were similar to the dependency in a PMMA phantom. The maximum CTDI difference between the PESR and PMMA phantoms was 7.5%. We conclude that the dose measured in the PESR phantom is similar to that in the PMMA phantom and that the PESR phantom can be used as an alternative if the PMMA phantom is not available.

摘要

本研究的目的是测量聚酯树脂(PESR)体模在不同管电压下的容积计算机断层扫描剂量指数(CTDI),并将其与标准聚甲基丙烯酸甲酯(PMMA)体模的值进行比较。两种体模均为直径16 cm的头部体模。使用CT扫描仪(GE Revolution EVO 64/128层)对体模进行扫描,管电压分别为80、100、120和140 kV。其他扫描参数保持恒定(即管电流为100 mA、旋转时间为1 s、准直宽度为10 mm)。通过将电离室插入体模内的五个孔中测量剂量来获得CTDI和CTDI。CTDI是根据CTDI和CTDI值计算得出的。每个孔的测量重复三次。结果发现,PESR体模的CTDI值取决于管电压值,并且与PMMA体模中的依赖性相似。PESR体模和PMMA体模之间的最大CTDI差异为7.5%。我们得出结论,在PESR体模中测量的剂量与在PMMA体模中测量的剂量相似,并且如果没有PMMA体模,PESR体模可以用作替代品。

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