• Journal of Radiation Protection and Research
• /
• 제46권3호
• /
• pp.127-133
• /
• 2021

Background: Phosphogypsum is material produced as a byproduct in fertilizer industry and is generally used for building materials. This material may contain enhanced radium-226 (²²⁶Ra) activity concentration compared to its natural concentration that may lead to indoor radon accumulation. Therefore, an accurate measurement method is proposed in this study to determine ²²⁶Ra activity concentration in phosphogypsum sample, considering the potential radon leakage from the sample container. Materials and Methods: The International Atomic Energy Agency (IAEA) phosphogypsum reference material was used as a sample in this study. High-purity germanium (HPGe) gamma spectrometry was used to measure the activity concentration of the ²²⁶Ra decay products, i.e., ²¹⁴Bi and ²¹⁴Pb. Marinelli beakers sealed with three different sealing methods were used as sample containers. Due to the potential leakage of radon from the Marinelli beaker (MB), correction to the activity concentration resulted in gamma spectrometry is needed. Therefore, the leaked fraction of radon escaped from the sample container was calculated and added to the gamma spectrometry measured values. Results and Discussion: Total activity concentration of ²²⁶Ra was determined by summing up the activity concentration from gamma spectrometry measurement and calculated concentration from radon leakage correction method. The results obtained from ²¹⁴Bi peak were 723.4 ± 4.0 Bq·kg^-1 in MB1 and 719.2 ± 3.5 Bq·kg^-1 in MB2 that showed about 5% discrepancy compared to the certified activity. Besides, results obtained from ²¹⁴Pb peak were 741.9 ± 3.6 Bq·kg^-1 in MB1 and 740.1 ± 3.4 Bq·kg^-1 in MB2 that showed about 2% difference compared to the certified activity measurement of ²²⁶Ra concentration activity. Conclusion: The results show that radon leakage correction was calculated with insignificant discrepancy to the certified values and provided improvement to the gamma spectrometry. Therefore, measuring ²²⁶Ra activity concentration in TENORM (technologically enhanced naturally occurring radioactive material) sample using radon leakage correction can be concluded as a convenient and accurate method that can be easily conducted with simple calculation.

• 대한방사선기술학회지:방사선기술과학
• /
• 제40권4호
• /
• pp.605-611
• /
• 2017

검출기의 구조를 PENELOPE의 코드를 사용하여 전산모사 하였다. 표준혼합시료(450, 1,000 ml)를 사용하여 다양한 밀도와 높이에 따른 저에너지(59.54 keV)부터 고 에너지(1,836.05)에 대한 측정효율과 PENELOPE 전산모사에서 구한 효율을 비교하였으며, 또한 자체흡수에 대한 효율을 보정하여 다양한 환경시료에 적용하여 검출하한치를 알아보고자 한다. 표준혼합선원의 전체에너지 피크효율 값을 적용하여 높이에 따른 효율변화를 측정치와 PENELOPE의 전산모사 값과 비교하였다. 여기서 구한 값들을 자체흡수 보정하여 구한 효율을 실제 환경시료에 적용하여 검출하한치 값들을 구하였다. 밀도보정인자는 밀도가 $0.4g/cm^3$에서 241Am(59.54 keV)의 밀도보정인자는 1.15, PENELOPE 전산모사에서는 1.153, 137CS(661.66 keV) 에서는 $1.06g/cm^3$, PENELOPE 전산모사에서는 1.064, 88Y(1,836.04 keV)에 대한 밀도보정인자는 1.03, PENELOPE 전산모사에서는 1.033으로 불확도는 1% 이내에서 잘 일치함을 확인하였다. 환경 시료의 밀도에 따른 방사능 농도는 시료량이 많을수록, 측정시간이 증가할수록 MDA(Minimum Detectable Activity) 값이 감소함을 확인할 수 있었다.

• Journal of Radiation Protection and Research
• /
• 제30권3호
• /
• pp.107-112
• /
• 2005

단일 핵종의 붕괴시 방출된 두 감마선이 함께 검출기에 흡수될 때 cascade summing이 일어난다. 이 효과는 일부 핵종에서 10% 이상의 계통적 오차를 야기한다. 이들 동시합성 효과를 추산하기 위해 검출기 주위에서 측정한 피크-토탈 비를 사용하여 그 효과를 직접 계산하였다. 검출기 주번에서 주어진 에너지에 대한 피크-토탈 비는 일정하지 않을 수 있으며, 따라서 측정된 값의 평균을 사용하여야 한다 산란 물체에 의한 피크-토달 비의 영향에 대한 결과도 함께 포함되어 있다.

• Nuclear Engineering and Technology
• /
• 제53권7호
• /
• pp.2348-2356
• /
• 2021

As a relatively new radiation imaging method, the cosmic-ray muon scattering imaging technology can be used to prevent nuclear smuggling and is of considerable significance to nuclear safety. Proposed in this paper is a new reconstruction algorithm based on density clustering, aiming to improve inspection quality with better performance. Firstly, this new algorithm is introduced in detail. Then in order to eliminate the inequity of the density threshold caused by the heterogeneity of the muon flux in different positions, a new flux correction method is proposed. Finally, three groups of simulation experiments are carried out with the help of Geant4 toolkit to optimize the algorithm parameters, verify the correction method and test the inspection quality under shielded condition, and compare this algorithm with another common inspection algorithm under different conditions. The results show that this algorithm can effectively identify and locate nuclear material with low misjudging and missing rates even when there is shielding and momentum precision is low, and the threshold correcting method is universally effective for density clustering algorithms.

• 한국의학물리학회:학술대회논문집
• /
• 한국의학물리학회 2006년도 제33회 추계학술대회 발표논문집
• /
• pp.68-68
• /
• 2006

• Nuclear Engineering and Technology
• /
• 제27권5호
• /
• pp.784-791
• /
• 1995

방사선계측에서는 방사선검출기(detector)로부터 나오는 pulse를 처리하는 데 있어서 pulse의 counting 손실이 발생한다. 이 손실을 최소화하거나 보상하기 위한 여러가지 방법들이 제시되어 왔으나, 아직도 절대적인 해답이 확립되지 않은 실정이다. 본 연구에서는 기 제시된 보상알고리즘들을 그 기능을 구현하는 전자회로와 함께 기술하고 특징을 분석하였다. 또한 본 연구를 통해 pulse의 counting손실을 보상하는 한가지 알고리즘 개선방향을 제시하였다.

• 융복합기술연구소 논문집
• /
• 제10권1호
• /
• pp.13-17
• /
• 2020

Among the factors that must be taken into account when using thermal imaging cameras that are expanding their application to various fields, a basic study was conducted focusing on temperature on the effect of solar radiation on the photographed thermal image. Through all experiments, in order to use an image taken with a thermal imaging camera for an object installed or located outdoors, a separate temperature correction according to the size of solar radiation or a separate device to block the effect of solar radiation must be additionally installed. Since the temperature of the same object may vary in the thermal image taken indoors or outdoors, it is necessary to calibrate it through comparison with other temperatures as a reference point. In the case of measuring the temperature of a glossy surface such as metal indoors with a thermal imaging camera, it was confirmed that an environment that can remove the light reflection effect by the glossy surface must be constructed and photographed.

• 한국의학물리학회지:의학물리
• /
• 제9권1호
• /
• pp.29-35
• /
• 1998

There has been necessity of an air free ionization chamber using the gold-crystal-aluminium plates, henceforth called the crystal chamber. The crystal chamber formed of parallel plates is very small in size and has more response for absorbed dose of therapeutic radiation beams. The gold plate on the crystal facing the photon and electron beam acts as an intensifier of signals and crystal plate as an ionization medium respectively. Both the copper guard ring and the aluminum collecting electrode are connected to an electrometer. Using high energy photon (6, 15 MV) and electron (9, 12, 15, 18 MeV) beams, the responses of the crystal chamber are evaluated against a PTW Farmer-type chamber at a field size of 10${\times}$10cm$^2$ and 100 cm SSD. The responses of crystal chamber for therapeutic radiation electron and photon beams are greater in magnitude by several order than Farmer. The crystal chamber has good linearity without correction factor C$\_$t,p/ with respect to the signals, a reading reproduction with good accuracy and precision less than 0.5%, and has other useful functions in measuring radiation beams.

• 한국의학물리학회지:의학물리
• /
• 제31권3호
• /
• pp.54-62
• /
• 2020

Dose calculation algorithms play an important role in radiation therapy and are even the basis for optimizing treatment plans, an important feature in the development of complex treatment technologies such as intensity-modulated radiation therapy. We reviewed the past and current status of dose calculation algorithms used in the treatment planning system for radiation therapy. The radiation-calculating dose calculation algorithm can be broadly classified into three main groups based on the mechanisms used: (1) factor-based, (2) model-based, and (3) principle-based. Factor-based algorithms are a type of empirical dose calculation that interpolates or extrapolates the dose in some basic measurements. Model-based algorithms, represented by the pencil beam convolution, analytical anisotropic, and collapse cone convolution algorithms, use a simplified physical process by using a convolution equation that convolutes the primary photon energy fluence with a kernel. Model-based algorithms allowing side scattering when beams are transmitted to the heterogeneous media provide more precise dose calculation results than correction-based algorithms. Principle-based algorithms, represented by Monte Carlo dose calculations, simulate all real physical processes involving beam particles during transportation; therefore, dose calculations are accurate but time consuming. For approximately 70 years, through the development of dose calculation algorithms and computing technology, the accuracy of dose calculation seems close to our clinical needs. Next-generation dose calculation algorithms are expected to include biologically equivalent doses or biologically effective doses, and doctors expect to be able to use them to improve the quality of treatment in the near future.

• 대한방사선치료학회지
• /
• 제19권1호
• /
• pp.1-5
• /
• 2007

목적: 방사선치료 시 OBI (on board imager) 시스템으로 환자 셋업 오차(set-up error)를 확인, 보정한 결과를 분석하여, 셋업 오차(set-up error)의 경향 및 원인을 살펴보고, 기존 필름과 EPID (electronic portal imaging device)를 사용한 방법에 비해 OBI의 정확성과 유용성에 대하여 알아보고자 한다. 대상 및 방법: 2006년 3월부터 2006년 5월까지 본원에 내원한 3차원 치료계획 환자 130명을 대상으로 주 1회 이상 OBI를 이용하여 치료전 셋업 영상의 분석을 시행하였다. 직각으로 획득한 2개의 영상을 모의 치료실에서 획득한 기준영상(reference image)과 합성(Fusion) 후 분석을 하였다. 분석 후 Vertical, Lateral, Longitudinal 방향으로 변위(Shift)거리를 측정하여 오차를 분석했다. 또한, 주요 부위별, 방향별로 구분하여 셋업 오차(set-up error) 요인들을 비교, 평가하였다. 결과: OBI를 적용하여 분석한 환자 41.5%에서 변위가 없이 Setup이 정확하였고, 52.3%에서 $1{\sim}5mm$정도의 오차가 존재하였다. 5 mm오차 이상인 환자도 6.1%가 확인되었다. 5 mm이상의 오차를 보인 환자들은 치료실내에서 확인한 결과 환자의 움직임이나 모의치료 자세와의 차이에서 오는 결과임을 알 수 있었다. 또한, 3 mm이상의 오차 경향이 3번 이상 지속될 경우에는 모의 치료실로 이동하여 보정후 치료를 시행하였다. 결론: 치료 전 2인의 근무자가 셋업을 정확히 하고 3면의 레이저와 조사야를 확인하였지만, 직각의 KV 영상으로 분석한 결과 셋업 오차가 발생할 수 있음을 확인하였다. 기존의 EPID에 의한 MV 영상은 낮은 영상의 특성과 환자의 피폭선량 증가라는 단점이 존재하지만, 본 연구에서 분석한 OBI는 모의 치료와 같은 높은 화질의 영상으로 셋업 오차의 정확한 계산과 객관적인 셋업 보정이 가능하여 영상유도 방사선치료의 정확도와 유용성을 입증할 수 있었다.