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Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination

The effective dose (H(E)) and organ or tissue equivalent dose (H(T)) for use in brain computed tomography (CT) examinations with various body weights were evaluated. Thermoluminescent dosimeters (TLD-100H) were inserted into Rando and five anthropomorphic phantoms. These phantoms were made of polyme...

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Autores principales: Lin, Hung-Chih, Lai, Te-Jen, Tseng, Hsien-Chun, Wang, Ching-Hsiang, Tseng, Yen-Ling, Chen, Chien-Yi
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Oxford University Press 2019
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6640898/
https://www.ncbi.nlm.nih.gov/pubmed/31197311
http://dx.doi.org/10.1093/jrr/rrz029
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author Lin, Hung-Chih
Lai, Te-Jen
Tseng, Hsien-Chun
Wang, Ching-Hsiang
Tseng, Yen-Ling
Chen, Chien-Yi
author_facet Lin, Hung-Chih
Lai, Te-Jen
Tseng, Hsien-Chun
Wang, Ching-Hsiang
Tseng, Yen-Ling
Chen, Chien-Yi
author_sort Lin, Hung-Chih
collection PubMed
description The effective dose (H(E)) and organ or tissue equivalent dose (H(T)) for use in brain computed tomography (CT) examinations with various body weights were evaluated. Thermoluminescent dosimeters (TLD-100H) were inserted into Rando and five anthropomorphic phantoms. These phantoms were made of polymethylmethacrylate (PMMA), according to the specifications of ICRU 48, with masses from 10 to 90 kg. Brain CT examinations were conducted, scanning the maxillae from the external auditory meatus to the parietal bone using a 128-slice multi-detector CT (MDCT) scanner. To reduce errors, three independent trials were conducted. Calculated H(E,TLD), based on the weighting factor recommended by ICRP 103, was 1.72 ± 0.28 mSv, which slightly exceeds the H(E,DLP) of 1.70 mSv, that was calculated from the dose–length product (DLP) of the Rando phantom. This experiment yielded H(E,TLD) values of ICRP 103 from the highest 1.85 ± 0.28 (90 kg) to the lowest 1.47 ± 0.22 (10 kg) mSv. H(E,TLD) (mSv) = 5.45×10(−3) W(kg) + 1.361, with an R(2) of 0.87667. Using the DLP protocol, H(E,DLP) was estimated from CTDI(vol) that was recorded directly from the console display of the CT unit and multiplied by the conversion coefficient (k) recommended by the ICRP 103. Finally, the experimental results obtained herein are compared with those in the literature. Physicians should choose and adjust protocols to prevent the exposure of patients to unnecessary radiation, satisfying the as low as reasonably achievable (ALARA) principle. These findings will be valuable to patients, physicians, radiologists and the public.
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spelling pubmed-66408982019-07-24 Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination Lin, Hung-Chih Lai, Te-Jen Tseng, Hsien-Chun Wang, Ching-Hsiang Tseng, Yen-Ling Chen, Chien-Yi J Radiat Res Regular Paper The effective dose (H(E)) and organ or tissue equivalent dose (H(T)) for use in brain computed tomography (CT) examinations with various body weights were evaluated. Thermoluminescent dosimeters (TLD-100H) were inserted into Rando and five anthropomorphic phantoms. These phantoms were made of polymethylmethacrylate (PMMA), according to the specifications of ICRU 48, with masses from 10 to 90 kg. Brain CT examinations were conducted, scanning the maxillae from the external auditory meatus to the parietal bone using a 128-slice multi-detector CT (MDCT) scanner. To reduce errors, three independent trials were conducted. Calculated H(E,TLD), based on the weighting factor recommended by ICRP 103, was 1.72 ± 0.28 mSv, which slightly exceeds the H(E,DLP) of 1.70 mSv, that was calculated from the dose–length product (DLP) of the Rando phantom. This experiment yielded H(E,TLD) values of ICRP 103 from the highest 1.85 ± 0.28 (90 kg) to the lowest 1.47 ± 0.22 (10 kg) mSv. H(E,TLD) (mSv) = 5.45×10(−3) W(kg) + 1.361, with an R(2) of 0.87667. Using the DLP protocol, H(E,DLP) was estimated from CTDI(vol) that was recorded directly from the console display of the CT unit and multiplied by the conversion coefficient (k) recommended by the ICRP 103. Finally, the experimental results obtained herein are compared with those in the literature. Physicians should choose and adjust protocols to prevent the exposure of patients to unnecessary radiation, satisfying the as low as reasonably achievable (ALARA) principle. These findings will be valuable to patients, physicians, radiologists and the public. Oxford University Press 2019-07 2019-06-14 /pmc/articles/PMC6640898/ /pubmed/31197311 http://dx.doi.org/10.1093/jrr/rrz029 Text en © The Author(s) 2019. Published by Oxford University Press on behalf of The Japan Radiation Research Society and Japanese Society for Radiation Oncology. http://creativecommons.org/licenses/by/4.0/ This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted reuse, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Regular Paper
Lin, Hung-Chih
Lai, Te-Jen
Tseng, Hsien-Chun
Wang, Ching-Hsiang
Tseng, Yen-Ling
Chen, Chien-Yi
Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination
title Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination
title_full Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination
title_fullStr Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination
title_full_unstemmed Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination
title_short Radiation doses with various body weights of phantoms in brain 128-slice MDCT examination
title_sort radiation doses with various body weights of phantoms in brain 128-slice mdct examination
topic Regular Paper
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC6640898/
https://www.ncbi.nlm.nih.gov/pubmed/31197311
http://dx.doi.org/10.1093/jrr/rrz029
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