• 제목/요약/키워드: Radiophotoluminescent glass dosimeter

검색결과 10건 처리시간 0.023초

Comparative Study of the Effective Dose from Panoramic Radiography in Dentistry Measured Using a Radiophotoluminescent Glass Dosimeter and an Optically Stimulated Luminescence Detector

  • Lee, Kyeong Hee;Kim, Myeong Seong;Kweon, Dae Cheol;Choi, Jiwon
    • 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.

A formalism for the absorbed dose evaluation of the glass dosimeter

  • Ka-Young Park;Hyun-Chul Kim;Byoung-Chul Kim
    • Nuclear Engineering and Technology
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    • 제55권6호
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    • pp.2283-2287
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    • 2023
  • We propose in the present work how the reference glass dosimeters can be introduced, which reflects the user irradiation condition. The reference glass dosimeters are used for correcting the reader fluctuation by reading it with sample glass dosimeters at the same time. Since they can be used without annealing after irradiation for long periods, one should consider both the fading effect and the natural background dose accumulation quantitatively. We construct an empirical but practical formalism of evaluating the absorbed dose on the glass dosimeter with the fading effect and the natural background dose accumulation considered.

엑스선의 조사시간에 따른 형광유리선량계의 빌드업 특성 (Buildup Characteristics of Radiophotoluminescent Glass Dosimeters with Exposure Time of X-ray)

  • 권대철
    • 대한의용생체공학회:의공학회지
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    • 제38권5호
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    • pp.256-263
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    • 2017
  • By using the buildup characteristics of the radiophotoluminescence glass dosimeter(RPLGD), it is aimed to help the measurement of the accurate dose by measuring the radiation dose according to the time of the glass element. Five glass elements were arranged on the table and the source to image receptor distance(SID) was set to 100 cm for the build-up radiation dose measurement of the fluorescent glass dosimeter glass element(GD-352M). Radiation doses and saturation rates were measured over time according to irradiation time, with the tube voltage (30, 60, 90 kVp) and tube current (50, 100 mAs) Repeatability test was repeated ten times to measure the coefficient of variation. The radiation dose increased from 0.182 mGy to 12.902 mGy and the saturation rate increased from 58.3% with increasing exposure condition and time. The coefficient of variation of the glass elements of the fluorescent glass dosimeter was ranged from 0.2 to 0.77 according to the X - ray exposure conditions. X - ray exposure showed that the radiation dose and saturation rate were increased with buildup characteristics, and degeneration of glass elements was not observed. The reproducibility of the variation coefficient of the radiation generator was included within the error range and the reproducibility of the radiation dose was excellent.

방사선 치료 시 산란선 및 누설선에 의한 표면선량 분포에 관한 연구 (A Study on the Surface Dose Distribution by Scattered and Leakage Radiation in Radiation Therapy)

  • 강종수;정동경;김용민
    • 한국방사선학회논문지
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    • 제12권3호
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    • pp.351-357
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    • 2018
  • 방사선 치료 시 환자는 부득이하게 산란선과 누설선에 의한 2차 방사선 피폭을 받게 된다. 진단용 방사선의 경우 진단참조준위로 환자의 피폭을 줄이기 위한 가이드라인을 제시하고 있지만 치료용 방사선의 경우 2차 방사선에 의한 피폭선량이 상당함에도 불구하고 상한치 설정 시 치료 효과의 저감을 이유로 선량을 제한하지 않고 있다. 이에 본 연구는 선형가속기를 이용한 방사선 치료 시 원거리 조직에서 환자가 받을 수 있는 2차 방사선을 형광유리선량계로 측정하였으며 형광유리선량계의 빌드업 특성에 따른 형광량의 포화도를 측정하였다. 연구 결과 조사야 경계로부터 거리가 멀어질수록 피폭선량은 급격히 줄어들었으며, 두부 1 Gy 조사 시 경부 18.45 mGy, 경부 1 Gy 조사 시 두부 15.55 mGy, 흉부 1 Gy 조사 시 경부 14.26 mGy, 골반 1 Gy 조사 시 흉부 1.14 mGy로 피폭되었다. 형광량의 포화도는 판독시점에 따라 1.8 ~ 4.8% 정도 과대평가 될 수 있음을 확인하였다.

Measurement uncertainty analysis of radiophotoluminescent glass dosimeter reader system based on GD-352M for estimation of protection quantity

  • Kim, Jae Seok;Park, Byeong Ryong;Yoo, Jaeryong;Ha, Wi-Ho;Jang, Seongjae;Jang, Won Il;Cho, Gyu Seok;Kim, Hyun;Chang, Insu;Kim, Yong Kyun
    • Nuclear Engineering and Technology
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    • 제54권2호
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    • pp.479-485
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    • 2022
  • At the Korea Institute of Radiological and Medical Sciences, physical human phantoms were developed to evaluate various radiation protection quantities, based on the mesh-type reference computational phantoms of the International Commission on Radiological Protection. The physical human phantoms were fabricated such that a radiophotoluminescent glass dosimeter (RPLGD) with a Tin filter, namely GD-352M, could be inserted into them. A Tin filter is used to eliminate the overestimated signals in low-energy photons below 100 keV. The measurement uncertainty of the RPLGD reader system based on GD-352M should be analyzed for obtaining reliable protection quantities before using it for practical applications. Generally, the measurement uncertainty of RPLGD systems without Tin filters is analyzed for quality assurance of radiotherapy units using a high-energy photon beam. However, in this study, the measurement uncertainty of GD-352M was analyzed for evaluating the protection quantities. The measurement uncertainty factors in the RPLGD include the reference irradiation, regression curve, reproducibility, uniformity, energy dependence, and angular dependence, as described by the International Organization for Standardization (ISO). These factors were calculated using the Guide to the Expression of Uncertainty in Measurement method, applying ISO/ASTM standards 51261(2013), 51707(2015), and SS-ISO 22127(2019). The measurement uncertainties of the RPLGD reader system with a coverage factor of k = 2 were calculated to be 9.26% from 0.005 to 1 Gy and 8.16% from 1 to 10 Gy. A blind test was conducted to validate the RPLGD reader system, which demonstrated that the readout doses included blind doses of 0.1, 1, 2, and 5 Gy. Overall, the En values were considered satisfactory.

유리선량계를 이용한 감마나이프의 출력인자 결정 (Determination of Output Factors for the Gamma Knife using a Radiophotoluminescent Glass Rod Detector)

  • 라정은;서원섭;신동오;김희선;서태석
    • 한국의학물리학회지:의학물리
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    • 제18권1호
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    • pp.13-19
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    • 2007
  • 본 연구에서는 유리선량계가 방사선 치료장비의 선량계로서의 적정성 여부를 확인하고자 감마나이프의 출력인자 및 X축 측방선량분포를 측정하였다. 출력인자는 가장 큰 콜리메이터인 18mm의 측정값을 기준으로 하여 14, 8 그리고 4mm에 대해 상대적으로 측정하였고 그 결과 각각 $0.980{\pm}0.013,\;0.949{\pm}0.013$ 그리고 $0.872{\pm}0.012$로 나타났다. 이는 제작회사에서 제공하고 있는 표준데이터와 모든 콜리메이터에서 1.0% 이내에서 잘 일치하는 결과이다. 또한 유리선량계로 측정한 4mm 콜리메이터의 x축 측방선량분포의 반치폭은 5.9mm였다.

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체외충격파쇄석술에서 투시 시 주요 장기별 방사선 피폭선량 (Radiation Dose during Fluoroscopy at the Organ from Extracorporeal Shock Wave Lithotripsy)

  • 문성호;정홍량;임청환
    • 한국콘텐츠학회논문지
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    • 제10권5호
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    • pp.343-350
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    • 2010
  • 체외충격파쇄석술(Extracorporeal shock wave lithotripsy ; ESWL) 시 환자가 받는 방사선 피폭선량을 측정하기 위하여 신장 및 요관 결석으로 진단을 받은 총 55명(남:36명, 여:19명)을 대상으로 방사선피폭선량을 측정하였다. 측정 방법은 투시 관전압 80kVp, 관전류 5mA로 고정하여 인체 모형의 Rando Phantom과 형광유리 선량계를 사용하였으며, 주요 장기인 양측 신장, 방광, 간에 5분과 10분씩 각각 2회 흡수선량을 측정하여 유효선량으로 환산하였다. 환자 당 평균 시행 횟수는 1.8회(1~4)이었고, 평균 투시시간은 533초(248~2516)로 나타났다. 우측 신장결석 치료 시 우측 신장의 평균값은 2.458mSv, 좌측 신장은 0.152mSv, 간은 1.404mSv, 방광은 0.019mSv로 측정 되었고, 좌측 신장결석 치료 시 좌측 신장의 평균값은 2.496mSv, 우측 신장은 0.252mSv, 간은 0.178mSv, 방광은 0.017mSv이었으며, 하부요관 결석치료 시 방광에서의 평균값은 3.742mSv, 우측 신장은 0.009mSv, 좌측 신장은 0.01mSv로 유효선량이 측정 되었다.

삼차원 뇌혈관조영술에서 테이블 높이와 확대율 조절에 따른 수정체 선량 감소에 대한 연구 (Radiation Dose Reduction of Lens by Adjusting Table Height and Magnification Ratio in 3D Cerebral Angiography)

  • 윤종태;이기백
    • 대한방사선기술학회지:방사선기술과학
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    • 제45권4호
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    • pp.313-320
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    • 2022
  • Both angiography and interventional procedures accompanied by angiography provide many diagnostic and therapeutic benefits to patients and are rapidly increasing. However, unlike general radiography or computed tomography using the same X-ray, the amount of radiation is quite high, but the dose range can vary considerably for each patient and operator. The high sensitivity of the lens to radiation during cerebral angiography and neurointervention is already well known, and although there are many related studies, it is insufficient to easily reduce radiation in diagnosis and treatment. In this situation, in particular, by adding three-dimensional rotational angiography (3D-RA) to the existing two-dimensional (2D) angiography, it is now possible to make an accurate diagnosis. However, since this 3D-RA acquires images through projection of more radiation than before, the exposure dose of the lens may be higher. Therefore, we tried to analyze whether the radiation dose of the lens can be reduced by moving the lens out of the field range by adjusting the table height and magnification ratio during the examination using 3D-RA. The surface dose was measured using a rando phantom and a radiophotoluminescent glass dosimeter (PLD) and the radiation dose was compared by adjusting the table height and magnification ratio based on the central point. As a result, it was found that the radiation dose of the lens decreased as the table height increased from the central point, that is, as the lens was out of the field of view. In conclusion, in 3D-RA, moving the table position of about 2 cm in height will make a significant contribution to the dose reduction of the lens, and it was confirmed that adjusting the magnification ratio can also reduce the surface dose of the lens.

유리선량계를 이용한 고에너지 전자선 측정 이용 가능성에 관한 연구 (Feasibility Study of the Radiophotoluminescent Glass Dosimeter for High-energy Electron Beams)

  • 손기홍;정해조;신상훈;이현호;이성현;김미숙;지영훈;김금배
    • 한국의학물리학회지:의학물리
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    • 제22권1호
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    • pp.52-58
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    • 2011
  • 본 연구에서는 유리선량계를 이용하여 전자선 치료빔의 선량평가 이용 가능성을 판단하고자 하였다. GD-302M 유리선량계에 선형가속기를 이용한 전자선과 $^{60}Co$ 방사선조사기로부터 감마선을 조사하였다. 유리선량계의 전자선에서의 선량 선형성, 재현성, 방향성, 선량률의존성, 에너지의존성의 총 5개 항목에 대해서 평가를 하였다. 측정은 물팬톰 $40{\times}40{\times}40cm^3$을 이용하여 유리선량계의 흡수선량을 측정하였다. 명목상 전자선에너지 6, 9, 12, 16, 20 MeV에서의 선량 1 Gy부터 15 Gy까지 유리선량계의 반응도를 평가해 본 결과 5개 전자선 에너지에서 같은 $R^2$=0.999의 선형계수를 확인할 수 있었다. 또한 5개의 에너지에서 총 100개의 유리선량계를 판독한 결과, 재현성은 5개 전자선에너지 평균 ${\pm}1.2%$ (1SD) 이내에서 잘 일치함을 확인할 수 있었다. 유리선량계의 방향성은 유리선량계의 수직방향인 $90^{\circ}$를 기준으로 하였을때 $0^{\circ}$에서 $90^{\circ}$사이에서 빔방향에 따라 1.5% 이내의 차이를 나타내었다. 선량률의존성은 500 MU/min을 기준으로 200 MU/min에서 1,000 MU/min 사이에서 ${\pm}1.5%$의 차이를 나타내었다. 유리선량계의 에너지 의존성은 원통형 전리함으로 측정한 선량과 비교했을때 5개의 명목상 전자선에너지(6 MeV에서 20 MeV) 각각에 대해 $^{60}Co$ 감마선의 반응도로 일반화시킨 결과 1.1%에서 3.5% 사이에서 낮은값을 나타내었다. 본 연구결과를 통하여 측정환경에 따라 결과값을 적절히 환산인자로 활용한다면 유리선량계를 이용한 전자선치료빔 선량평가가 가능하리라 사료된다.