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Monte Carlo 시뮬레이션과 3D Printing Phantom을 이용한 99mTc, 18F 선원 핵의학 검사 시 내부피폭 선량평가

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Alternative Title
Evaluation of Internal Exposure for Nuclear Medicine Study of 99mTc, 18F Sources using Monte Carlo Simulation and 3D printing phantom
Abstract
Nuclear medicine is a diagnostic field of anatomical and physiological state on the human body by using radioisotope. As the number of nuclear medicine imaging have been increased, the medical exposure involved inevitably. The radiation used is difficult to defend against enters the human body and provides many harmful effects. In particular, radiation detection equipment is difficult to accurately measure the internal exposure dose. In addition, accurate measurement of internal exposure is difficult because the characteristics vary depending on the nuclide and radioactive source. Although the reduction of radiation dose was studied in the past studies, the estimation of radiation in radiation workers and caregivers was not studied. In this study, the dose distribution of the human body was evaluated through dosimetry data using a water phantom, ionization chamber, photoluminescence glass dosimeter and Monte carlo simulation for 99mTc and 18F sources, which are frequently used in nuclear medicine. To evaluate whether the dose limit was exceeded, the lens absorbed dose was calculated using a brain phantom made by a 3d printer.
Absorbed dose rate(mGy/h) was respectively measured in a section of 3 ∼ 13 cm from the radioisotope(99mTc, 18F) of 10 mCi. The absorbed dose rate of 99mTc was shown in the range of 2.80 ∼ 0.35 mGy/h in the ionization chamber, 3.17 ∼ 0.36 mGy/h in the photoluminescence glass dosimeter and 3.18 ∼ 0.31 mGy/h in Monte carlo simulation. Under 18F radiation, the absorbed dose rates were gauged in the range of 24.4 ∼ 11.30 mGy/h in the ionization chamber, 25.79 ∼1.65 mGy/h in the photoluminescence glass dosimeter and 26.08 ∼ 1.42 mGy/h in Monte carlo simulation, respectively. From these results, it was confirmed that the higher radiation dose, the higher absorbed dose rate proportionally. Utilization of 18F source, which has relatively high energy, showed higher absorbed dose rate than that of 99mTc source. Also, the absorbed dose rate decreased exponentially with increase of the distance from the radioisotope. Especially, these results showed a tendency to decrease rapidly when the distance from the radioisotope increased over 5 cm. These results indicate that a large amount of dose is delivered to an organ located within 4 cm of source’s movement path when a source is an uptake in the human body.
In the 3d printing brain phantom study, the average absorbed dose rates for the left and right lenses based on 10 mCi of 99mTc and 18F were 3.37 and 28.62 mGy/h, respectively. The calculated values using the Monte carlo simulation were 3.72 and 28.86 mGy/h, respectively. In comparison with actual measurement and simulation results, 99mTc showed a difference of about 10% and 18F showed a difference of less than 1%. These differences originated from differences in measurement environment and simulation conditions such as the structure of brain phantom, radiation volume and specific radioactivity in this study.
Finally, the lens absorbed dose rate measured in the brain phantom is converted to a value that the effective half-life has elapsed 10 times. The absorbed dose was calculated by referring to the brain distribution fraction of biokinetic data for makers of HM-PAO and FDG in ICRP 80 and 53. As a result, the exposure dose to the lens was 1.16 mGy in the brain perfusion SPECT using 99mTc-HM-PAO 10 mCi, and the exposure dose to the lens in the PET torso using 18F-FDG 10 mCi was 3.46 mGy. These results satisfy the annual cap on the equivalent dose to the lens of the Korean Nuclear Safety Act(150 mSv). Also, these results fulfill the condition of the annual dose limit for the public in the recently revised ICRP 118(15 mSv). The importance of the dose limit for the lens become gradually emerging, and data on the radiation sensitivity of the lens are being derived. Therefore, various types of research have been conducted to reduce lens exposure in the diagnostic radiation field. To reduce lens exposure during brain CT, using shielding material made of bismuth and tungsten filament or scanning baseline change is suggested. In nuclear medicine, this study is an important data to determine whether the amount of radioactivity is appropriate by complying with the dose standards of radiopharmaceuticals according to the Diagnostic Reference Levels (DRLs) of nuclear medicine.
This study presented reliable results by comparing the actual measurement and Monte carlo simulation results to quantitatively evaluate the internal exposure dose by radioisotope. In conclusion, this study is considered to be helpful as basic data for setting the diagnostic reference level for nuclear medicine.
Author(s)
지영식
Issued Date
2023
Awarded Date
2023-02
Type
Dissertation
Keyword
핵의학 검사, 내부피폭, 체내 선량분포
Publisher
부경대학교
URI
https://repository.pknu.ac.kr:8443/handle/2021.oak/32955
http://pknu.dcollection.net/common/orgView/200000667180
Alternative Author(s)
Young Sik Ji
Affiliation
부경대학교 대학원
Department
대학원 인공지능융합학과
Advisor
양현경
Table Of Contents
1. 서론 1
2. 배경이론 3
2.1 방사선과 물질과의 상호작용 3
2.1.1 전자파 방사선과 물질과의 상호작용 4
2.1.2 전자와 물질과의 상호작용 9
2.1.3 중성자와 물질과의 상호작용 12
2.2 의료피폭 15
2.3 방사선 방호 체계 18
2.3.1 방호 기본원칙 18
2.3.2 방호의 원리 22
2.3.3 방사선량 25
2.4 핵의학과 사용 방사성동위원소 30
2.4.1 99mTc 32
2.4.2 18F 34
2.5 의료방사선에서 사용되는 팬텀 35
2.6 3D 프린팅 기술 37
2.6.1 3D 프린터의 기본 원리 37
2.6.2 3D 프린터의 종류 39
2.7 이온전리함 41
2.8 유리선량계 42
2.9 Monte Carlo 시뮬레이션 43
3. 실험방법 46
3.1 물 팬텀과 이온전리함을 이용한 실측실험 46
3.2 물 팬텀과 유리선량계를 이용한 실측실험 51
3.2.1 유리선량계의 판독 53
3.3 물 팬텀 내 선량분포의 Monte Carlo 시뮬레이션 56
3.4 3D 프린터를 이용한 뇌 팬텀 제작과 유리선량계를 이용한 실측실험 58
3.4.1 3D 프린터를 이용한 뇌 팬텀 제작 58
3.4.2 뇌 팬텀을 이용한 수정체 실측실험 62
3.5 뇌 팬텀과 수정체 선량분포의 Monte Carlo 시뮬레이션 63
3.6 수정체 실측실험 결과와 ICRP의 흡수선량 비교 68
4. 실험결과 및 고찰 69
4.1 물 팬텀과 이온전리함을 이용한 실험결과 69
4.1.1 99mTc 선원의 거리에 따른 선량분포 69
4.1.2 18F 선원의 거리에 따른 선량분포 73
4.2 물 팬텀과 유리선량계를 이용한 실험결과 76
4.2.1 99mTc 선원의 거리에 따른 선량분포 76
4.2.2 18F 선원의 거리에 따른 선량분포 79
4.3 물 팬텀 내 선량분포의 Monte Carlo 시뮬레이션 결과 82
4.3.1 99mTc 선원의 거리에 따른 선량분포 82
4.3.2 18F 선원의 거리에 따른 선량분포 83
4.4 물 팬텀 실측실험과 Monte Carlo 시뮬레이션 결과 비교 84
4.4.1 99mTc 선원 10 mCi 실측실험과 Monte Carlo 시뮬레이션 결과 비교 84
4.4.2 18F 선원 10 mCi 실측실험과 Monte Carlo 시뮬레이션 결과 비교 86
4.5 뇌 팬텀의 수정체 실측실험 결과 88
4.5.1 99mTc 선원의 수정체 실측실험 결과 88
4.5.2 18F 선원의 수정체 실측실험 결과 90
4.6 뇌 팬텀과 수정체 선량 분포의 Monte Carlo 시뮬레이션 결과 92
4.7 뇌 팬텀 실측실험과 Monte Carlo 시뮬레이션 결과 비교 93
4.8 수정체 실측실험 결과와 ICRP 흡수선량 결과 비교 95
5. 결론 97
참고문헌 99
Degree
Doctor
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