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The effects of mis-centering on radiation dose during CT head examination: A phantom study

机译:误导对CT头检测期间辐射剂量的影响:幻影研究

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There are several factors that may contribute to the increase in radiation dose of CT including the use of unoptimized protocols and improper scanning technique. In this study, we aim to determine significant impact on radiation dose as a result of mis-centering during CT head examination. The scanning was performed by using Toshiba Aquilion 64 slices multidetector CT (MDCT) scanner and dose were measured by using calibrated ionization chamber. Two scanning protocols of routine CT head; 120 kVp/ 180 mAs and 100 kVp/ 142 mAs were used represent standard and low dose, respectively. As reference measurement, the dose was first measured on standard cylindrical polymethyl methacrylate (PMMA) phantom that positioned at 104 cm from the floor (reference isocenter). The positions then were varied to simulate mis-centering by 5 cm from isocenter, superiorly and inferiorly at 109 cm, 114 cm, 119 cm, 124 cm and 99 cm, 94 cm, 89 cm, 84 cm, respectively. Scanning parameter and dose information from the console were recorded for the radiation effective dose (E) measurement. The highest mean CTDIvol value for MCS and MCI were 105.06 mGy (at +10 cm) and 105.51 mGy (at -10 cm), respectively which differed significantly (p < 0.05) as compared to the isocenter. There were large significant different (p < 0.05) of mean Dose Length Product (DLP) recorded between isocenter to the MCS (85.8 mGy.cm ) and MCI (93.1 mGy.cm ). As the low dose protocol implemented, the volume CTDI (CTDIvol) were significantly increase (p < 0.05) for MCS (at +10 cm) and MCI (at -10 cm) when compared to the isocenter. The phantom study revealed a noticeable different in radiation dose between isocenter and experimental groups due to degradation of the bowtie filter performance. It is anticipated that these noteworthy findings may emphasize the importance of accurate patient centering at the isocenter of CT gantry, so that CT optimization practice can be achieved.
机译:有几个因素可能导致CT的辐射剂量的增加,包括使用未优化的协议和不当扫描技术。在这项研究中,我们的目的是在CT头检查期间误导时对辐射剂量进行显着影响。通过使用TOSHIBA Aquilion 64切片来执行扫描,通过使用校准电离室测量扫描仪和剂量。两种扫描协议的常规CT头;使用120 kVP / 180 MAS和100 kVP / 142 MAS分别代表标准和低剂量。作为参考测量,首先在从地板(参考等中心)以104cm处的标准圆柱形聚甲基丙烯酸甲酯(PMMA)幻体上测量剂量。然后将位置变化以将偏心5厘米从Isocenter进行了5厘米,优于109cm,114cm,119cm,124cm和99cm,94cm,89cm,84cm。记录从控制台的扫描参数和剂量信息用于辐射有效剂量(E)测量。 MCS和MCI的最高平均CTDIVOL值分别为105.06 mgy(+10厘米)和105.51米(在-10cm),与ISOcenter相比,显着不同(P <0.05)。在Isocenter到MCS(85.8 MGY.cm)和MCI(93.1 MGY.cm)之间的平均剂量长度产品(P <0.05)的平均剂量长度产品(DLP)存在大。随着低剂量方案所实施的,与等离心相比,MCS(+10cm)和MCI(在-10cm)显着增加(P <0.05)。 Phantom研究表明,由于弓形滤光器性能的降解,Isocenter和实验组之间的辐射剂量中显着不同。预计这些值得注意的发现可以强调准确患者在CT龙门的Isocenter上定心的重要性,从而可以实现CT优化实践。

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