• Journal of Radiation Protection and Research
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• 제36권3호
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• pp.127-133
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• 2011

국제방사선방호위원회에서는 2007년에 방사선방호에 관한 권고(ICRP 103)를 개정하였다. 이에 따라 국제원자력기구에서도 전리방사선 방호에 관한 국제기본안전기준을 개정하고 있으며 국내에서도 신권고의 내용을 국내요건에 반영하기 위한 연구가 진행 중이다. 신권고가 기존 권고에서 크게 변화되지 않았지만 방사선산업의 성장으로 인해 작은 변화에도 큰 영향을 가져올 수 있기 때문에 신권고의 내용을 국내 반영하기 위한 준비가 필요하다. ICRP 103의 주요 특징중 하나는 기존 권고에 비해 방호최적화를 한 단계 더 강조한 것이다. 이를 위해 계획피폭상황에서 선량제약치를, 기존 및 비상피폭상황에서 참조준위를 사용할 것을 권고하였다. 선량제약치는 전망적이고 선원중심적 제한값으로서 개인에 대한 방호의 기본 수준을 제공하며, 그 선원에 대한 방사선방호 최적화에 상한 선량 역할을 하게 된다. 이에 따라 국내에서도 원자력 및 방사선이용시설에 대해 선량제약치 운영이 요구될 것이다. 규제기관과의 협력과 더불어 직무피폭에 관한 선량제약치를 사업자가 설정하고 운영함으로써 최적화가 더 강조될 수 있을 것으로 예상된다. 선량제약치가 규제도구가 아닌 방사선방호최적화를 위한 절차로 국내 적용되기 위한 방안을 도출하였다.

• 방사선산업학회지
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• 제17권1호
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• pp.111-118
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• 2023

The International Commission on Radiological Protection (ICRP) 103 recommends a cost-benefit analysis method as an auxiliary tool for scientific and rational decision-making for the principle of optimization of radiological protection. In order to conduct a cost-benefit analysis, the safety improvement of nuclear power by regulation must be measured and converted into monetary terms. The improvement of nuclear safety can be measured by reducing the radiation exposure dose of the people, and it is necessary to determine the coefficient to convert the radiation exposure dose into money. The monetary coefficient is calculated as the product of the statistical life value (VSL) and the nominal risk coefficient. In order to derive the monetary coefficient, the willingness to pay (WTP) can be estimated using the contingent valuation method (CVM), which quantifies the value of non-market goods by converting them into monetary units. WTP can be estimated based on the random utility model, which is the basic model for bivariate selection type conditional value measurement data. Statistical life value can be calculated using the estimated WTP and reduction in early mortality, and a monetary coefficient can be derived.

• Journal of Radiation Protection and Research
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• 제36권3호
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• pp.154-159
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• 2011

국내 원전에서는 고 방사선량율 또는 고피폭 예상 방사선작업에 종사자의 가슴과 등에 두 개의 개인선량계를 패용하여 피폭방사선량을 평가하고 있다. 이러한 Two-Dosimeter Algorithm (TDA)으로 현장시험과 심층검토를 통해 NCRP(55:50) TDA를 최적 알고리즘으로 최종적으로 선정하였고, 2006년 이후 원전 종사자의 피폭방사선량 평가 실무에 적용 중에 있다. 한편, 2007년 국제방사선방호위원회(ICRP)는 간행물 ICRP 103을 통해 방사선가중계수 및 조직가중계수와 기준 인체모형팬텀(Reference phantom) 등을 일부 변경한 유효선량 평가방법을 제시하였다. 이에 따라 본 논문에서는 국내원전에서 적용되고 있는 NCRP (55:50) TDA에 대해 ICRP 103 방사선방호 체계 하에서의 계속 적용 타당성을 분석하였다. 그 결과, NCRP (55:50) TDA를 계속 사용하더라도 ICRP 103의 유효선량을 신뢰성 있게 평가할 수 있는 것으로 판단되었다.

• 대한디지털의료영상학회논문지
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• 제14권2호
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• pp.9-14
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• 2012

Exposed dose of young child should be managed necessarily. Young child is more sensitive than adult of a Radioactivity, especially, and lives longer than adult. Must reduce exposed dose which follows The ALARA(As Low As Reasonably Achievable)rule is recommended by ICRP(International Commission on Radiological Protection)within diagnostic useful range. Therefore, We have to prepare Pediatric DRL(Diagnostic Reference Level) in Korea as soon as possible. Consequently, in this study, wish to estimate organ dose and effective dose using PCXMC Program(a PC-Based Monte Carlo Program), and measure ESD(Entrance surface dose)and organ dose using Glass dosimeter, and then compare with DRL which follows EC(European Commission)and NRPB(National Radiological Protection Board). Using glass dosimeter and PCXMC programs conforming to the International Committee for Radioactivity Prevention(ICRP)-103 tissue weighting factor based on the item before the organs contained in the Chest, Skull, Pelvis, Abdomen in the organ doses and effective dose and dose measurements were evaluated convenience. In a straightforward way to RANDO phantom inserted glass dosimeter(GD352M)by using the hospital pediatric protocol, and in a indirect way was PCXMC the program through a virtual simulation of organ doses and effective dose were calculated. The ESD in Chest PA is 0.076mGy which is slightly higher than the DRL of NRPB(UK) is 0.07mGy, and is lower than the DRL of EC(Europe) which is 0.1mGy. The ESD in Chest Lateral is 0.130mGy which is lower than the DRL of EC(Europe) is 0.2mGy. The ESD in Skull PA is 0.423mGy which is 40 percent lower than the DRL of NRPB(UK) is 1.1mGy and is 28 percent lower than the DRL of EC(Europe) is 1.5mGy. The ESD in Skull Lateral is 0.478mGy which is half than the DRL of NRPB(UK) is 0.8mGy, is 40 percent lower than the DRL of EC(Europe) is 1mGy. The ESD in Pelvis AP is 0.293mGy which is half than the DRL of NRPB(UK) is 0.60mGy, is 30 percent lower than the DRL of EC(Europe)is 0.9mGy. Finally, the ESD in Abdomen AP is 0.223mGy which is half than the DRL of NRPB(UK) is 0.5mGy, and is 20 percent lower than the DRL of EC is 1.0mGy. The six kind of diagnostic radiological examination is generally lower than the DRL of NRPB(UK)and EC(Europe) except for Chest PA. Shouldn't overlook the age, body, other factors. Radiological technician must realize organ dose, effective dose, ESD when examining young child in hospital. That's why young child is more sensitive than adult of a Radioactivity.

• 한국방사선학회논문지
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• 제18권5호
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• pp.403-409
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• 2024

본 연구에서는 인천광역시 내 C 대학병원의 의료기관에서 근무하는 방사선 작업종사자들과 임상실습에 임하는 방사선학과 재학생들의 피폭선량을 측정하고, 발생률을 분석함으로써 방사선의 확률적 영향에 관련하여 기초자료를 제공하고자 하였다. 2023년 1월 1일부터 12월 31일까지 인천광역시 내 C 대학병원 방사선 작업종사자 구역에서 근무한 핵의학과(10명)와 방사선종양학과(15명) 방사선사들과 동 의료기관에서 7~8 월 임상 실습과정을 모두 이수한 방사선학과 재학생 82명을 연구대상으로 하였다. 방사선종양학과 방사선사들의 피폭선량으로 인한 폐의 부작용 발생률은 표층선량과 심부선량은 모두 10,000,000명 당 2.5명의 확률임을 나타내었다. 핵의학과는 표층선량 2.90 ± 0.61 mSv, 심부선량은 3.02 ± 0.63 mSv로 100,000명 당 1.5명이 발생확률임을 나타내었다. 그리고 수시출입자로 분류된 방사선학과 재학생들은 표층선량은 0.99 ± 0.12 mSv, 심부선량은 0.97 ± 0.11 mSv 였으며 발생확률은 1,000,000명 당 6.8명, 6.6명의 결과를 산출하였다. 방사선 종사자들의 개인별 피폭선량을 최소화하며 방사선의 안전관리와 확률적 영향을 분석하기 위한 기초자료가 되리라 사료된다.

• Journal of the Korean Physical Society
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• 제73권9호
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• pp.1377-1384
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• 2018

Accurate measurement of the absorbed dose and the effective dose is required in dental panoramic radiography involving relatively low energy with a rotational X-ray tube system using long exposures. To determine the effectiveness of measuring the irradiation by using passive dosimetry, we compared the entrance skin doses by using a radiophotoluminescent glass dosimeter (RPL) and an optically stimulated luminescence detector (OSL) in a phantom model consisting of nine and 31 transverse sections. The parameters of the panoramic device were set to 80 kV, 4 mA, and 12 s in the standard program mode. The X-ray spectrum was applied in the same manner as the panoramic dose by using the SpekCalc Software. The results indicated a mass attenuation coefficient of $0.008226cm^2/g$, and an effective energy of 34 keV. The equivalent dose between the RPL and the OSL was calculated based on a product of the absorbed doses. The density of the aluminum attenuators was $2.699g/cm^3$. During the panoramic examination, tissue absorption doses with regard to the RPL were a surface dose of $75.33{\mu}Gy$ and a depth dose of $71.77{\mu}Gy$, those with regard to the OSL were surface dose of $9.2{\mu}Gy$ a depth dose of $70.39{\mu}Gy$ and a mean dose of $74.79{\mu}Gy$. The effective dose based on the International Commission on Radiological Protection Publication 103 tissue weighting factor for the RPL were $0.742{\mu}Sv$, $8.9{\mu}Sv$, $2.96{\mu}Sv$ and those for the OSL were $0.754{\mu}Sv$, $9.05{\mu}Sv$, and $3.018{\mu}Sv$ in the parotid and sublingual glands, orbit, and thyroid gland, respectively. The RPL was more effective than the OSL for measuring the absorbed radiation dose in low-energy systems with a rotational X-ray tube.

• 방사선산업학회지
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• 제17권1호
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• pp.61-67
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• 2023

A Study on the Introduction of Dose Constraints for Occupational Exposures: Focusing on Experts' Opinions by Field of Radiation Industry. The International Commission on Radiological Protection suggests Justification, Optimization, and Dose Limits as the three principles of radiological protection, among which, as a means of protection optimization, ICRP 103 recommends to set dose constraints. In this study, opinions are collected from experts in each category of radiation industries for stakeholder participation to qualify dose constraints. A guidance and questionnaire for analyzing the dose constraints have been developed for their collection, and opinions were collected from radiation protection experts in selected categories. 20 out of 22 experts, consisted with 91%, have assessed the dose constraints setting is necessary, and 2 experts, consisted with 9%, assessed it is unnecessary. The average of dose constraint presented by experts for RI production institutions is to be the highest level of 15.3 mSv, and light-water reactors (14.6 mSv), non-destructive inspection (14.4 mSv), heavy-water reactor and medical institutes (13.9mSv) is to be above the overall average dose constraint. In case of public institutions, the average dose constraint is to be 8.6mSv, and research institutions (8.8mSv), educational institutions (9.6 mSv), waste disposal sites (9.7 mSv), and general industries (10.6 mSv) are resulted to below the overall average dose constraint. As for the means of setting dose constraints, 8 experts out of 22 suggested setting dose constraints for each specific industry or task. And, 5 experts especially suggest setting dose constraints for the specific groups with relatively high exposure, such as workers with above the record levels. As a countermeasure for workers who exceed the dose constraints, 15 experts out of 22 expressed that the cause analyses for them and preparation for a plan of reducing them are necessary.

• 한국방사선학회논문지
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• 제18권4호
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• pp.383-389
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• 2024

본 연구에서 전립샘암의 방사선치료기법 중 세기조절 방사선 치료 시 정상장기인 복부의 광중성자 피폭으로 인하여 2차 암이 발생할 확률을 분석하고자 한다. 전립샘암 방사선 치료계획의 설계는 일일 처방선량 220 cGy, 총 치료 횟수는 35회로 7700 cGy로 수립하였다. 실험장비는 Varian 사의 True Beam STx(Varian, USA) 선형가속기이다. 실험에 사용한 에너지는 15 MV로 치료 계획용 표적체적(Planning target volume; PTV)안에 광중성자 선량이 발생하도록 치료계획을 설계하였다. 방사선 치료계획은 Eclipse System (Varian Ver 10.0, USA)이며, 조사문수를 5 ~ 9개로 설정하였다. 조사각도는 0° ~ 320°에서 처방선량(prescription dose)영역에 95%가 설정되도록 설계하였으며, 각각의 조사문수당 소조사면(beamlet)은 100개로 설정하였다. 광중성자의 선량 측정을 위하여 본 연구에 사용한 광자극발광선량계는 알류미늄산화물 성분이 포함된 소자에 ⁶LiCO₃ 를 도포하여 중성자 선량이 측정 가능하도록 설계하였다. 세기조절 방사선 치료 시 복부의 광중성자 선량으로 인하여, 1,000명 기준으로 최소 7.07 ~ 11명이 2차 암의 발생확률이 있음이 연구되었다. 본 연구에서 세기조절 방사선치료 시 발생될 수 있는 2차 피폭선량의 위험성을 연구하여, 추후 방사선의 확률적 영향과 관련된 의미 있는 자료로 활용되기를 기대한다.

• 한국안전학회지
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• 제31권5호
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• pp.22-27
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• 2016

The Electrostatic Charge Prevention Technology is a core factor that highly influences the yield of Ultra High Resolution Flat Panel Display and high-integrated semiconductor manufacturing processes. The corona or x-ray ionizations are commonly used in order to eliminate static charges during manufacturing processes. To develop such a revolutionary x-ray ionizer that is free of x-ray radiation and has function to control the volume of ion formation simultaneously is a goal of this research and it absolutely overcomes the current risks of x-ray ionization. Under the International Commission on Radiological Protection, it must have a leakage radiation level that should be lower than a recommended level that is $1{\mu}Sv/hour$. In this research, the new generation of x-ray ionizer can easily control both the volume of ion formation and the leakage radiation level at the same time. In the research, the test constraints were set and the descriptions are as below; First, In order not to leak x-ray radiation while testing, the shielding box was fully installed around the test equipment area. Second, Implement the metallic Ring Electrode along a tube window and applied zero to ${\pm}8kV$ with respect to manage the positive and negative ions formation. Lastly, the ion duty ratio was able to be controlled in different test set-ups along with a free x-ray leakage through the metallic Ring Electrode. In the result of experiment, the maximum x-ray radiation leakage was $0.2{\mu}Sv/h$. These outcome is lower than the ICRP 103 recommended value, which is $1{\mu}Sv/h$. When applying voltage to the metallic ring electrode, the positive decay time was 2.18s at the distance of 300 mm and its slope was 0.272. In addition, the negative decay time was 2.1s at the distance of 300 mm and its slope was 0.262. At the distance of 200 mm, the positive decay time was 2.29s and its slope was 0.286. The negative decay time was 2.35s and its slope was 0.293. At the distance of 100 mm, the positive decay time was 2.71s and its slope was 0.338. The negative decay time was 3.07s and its slope was 0.383. According to these research, the observation was shown that these new concept of ionizer is able to minimize the leakage radiation level and to control the positive and negative ion duty ratio while ionization.