• ETRI Journal
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• 제46권2호
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• pp.175-183
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• 2024

Recently, polar code has attracted the attention of many scholars and has been developed as a code technology in coded-cooperative communication. We propose a polar code scheme based on Plotkin structure and quasi-uniform punching (PC-QUP). Then we apply the PC-QUP to coded-cooperative scenario and built to a new coded-cooperative scheme, which is called PCC-QUP scheme. The coded-cooperative scheme based on polar code is studied on the aspects of codeword construction and performance optimization. Further, we apply the proposed schemes to space-time block coding (STBC) to explore the performance of the scheme. Monte Carlo simulation results show that the proposed cooperative PCC-QUP-STBC scheme can obtain a lower bit error ratio (BER) than its corresponding noncooperative scheme.

• Nuclear Engineering and Technology
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• 제52권8호
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• pp.1603-1610
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• 2020

Due to ever-growing advancements in computers and relatively easy access to them, many efforts have been made to develop high-fidelity, high-performance, multi-physics tools, which play a crucial role in the design and operation of nuclear reactors. For this purpose in this study, the neutronic Monte Carlo and thermal-hydraulic sub-channel codes entitled MCNP and COBRA-EN, respectively, were applied for external coupling with each other. The coupled code was validated by code-to-code comparison with the internal couplings between MCNP5 and SUBCHANFLOW as well as MCNP6 and CTF. The simulation results of all code systems were in good agreement with each other. Then, as the second problem, the core of the VVER-1000 v446 reactor was simulated by the MCNP4C/COBRA-EN coupled code to measure the capability of the developed code to calculate the neutronic and thermohydraulic parameters of real and industrial cases. The simulation results of VVER-1000 core were compared with FSAR and another numerical solution of this benchmark. The obtained results showed that the ability of the MCNP4C/COBRA-EN code for estimating the neutronic and thermohydraulic parameters was very satisfactory.

• 한국콘텐츠학회논문지
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• 제14권2호
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• pp.467-474
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• 2014

MCNPX를 통하여 계산한 상대선량과 고체팬텀과 전리함을 이용하여 측정한 상대선량을 비교하여 몬테카를로 시뮬레이션의 정확성을 평가하였다. 그리고 간외 담도암 관내근접방사선치료를 몬테카를로 시뮬레이션에 적용하기 위해 192Ir 밀봉방사성선원을 모사하였고, 한국 성인남성 표준인을 기초로 하는 KMIRD형 팬텀을 이용하여 담도 및 주변 장기를 제작하였다. 간외 담도암 관내근접방사선치료를 MCNPX를 이용하여 담도 주변 정상장기의 비유효에너지와 초기방사능을 1 Ci로 설정하여 흡수선량을 산정하였다. 몬테카를로 시뮬레이션의 정확성 평가에서 상대선량 차이가 가장 많은 지점이 1.96%로 MCNPX에서 제시한 상대오차 2%를 만족하는 것으로 나타났다. 또한, 담도 주변 정상장기의 비유효에너지 및 흡수선량은 담도와비교적 인접한 위치에 있는 우측신장, 간, 췌장, 횡행결장, 척수, 위장, 소장이 높았고, 담도와의 거리가 떨어져 있는 장기들인 좌측신장, 비장, 상행결장, 하행결장, S상결장이 낮게 나타났다.

• Journal of Radiation Protection and Research
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• 제26권3호
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• pp.271-273
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• 2001

In precise measurement of air kerma with cavity ionization chambers, the effect of wall attenuation and scatter are corrected by Kwall and that of nonuniformity by Knu. Using the EGS4 code, we calculated these two correction factors. Correction factors calculated for two different-sized cylindrical ionization chamber differ by up to 0.7% from those obtained by measurements.

• Nuclear Engineering and Technology
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• 제54권7호
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• pp.2572-2578
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• 2022

An approximate method for calculating the cadmium ratio of a cyclotron-based thermal neutron radiography system was developed. In this method, the Monte-Carlo code, MCNP6.2, was employed to calculate the neutron capture rates of Au-197, and the cadmium ratio was obtained by computing the ratio of neutron capture rates. From the simulation results, the computed cadmium ratio is reasonably acceptable, and the assumption of ignoring the fast neutron contribution to the cadmium ratio is valid.

• Journal of Radiation Protection and Research
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• 제32권1호
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• pp.21-26
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• 2007

본 논문은 몬테칼로 시뮬레이션을 이용하여 대단위 감마선 조사시설 (IR-221)에 대한 선량률 평가 및 선량 분포를 해석하고, 이러한 방법을 통해 방사선 조사 품질을 향상시키는 것을 목적으로 하고 있다. 몬테칼로 시뮬레이션은 MCNP4B 코드를 이용하여 계산하였고, 이를 검증하기 위해 알라닌 선량계를 이용하여 전체 309개 지점에 대하여 흡수선량을 측정하였다. 계산 값과 측정치의 차이는 대략 ${\pm}5%$범위를 벗어나지 않음으로써 MCNP4B 코드가 IR-221 감사선 조사시설의 선량분포를 해석하는데 있어서 유효한 수단임을 알 수 있었다. 감마선 조사시설에 대한 도시메트리는 보통 많은 인력과 시간을 필요로 하지만, 몬테칼로 계산을 통해 이러한 손실을 줄일 수 있고, 무엇보다도 방사선 조사 품질을 향상시켜, 결국 방사선 조사 대상물에 대한 신뢰도를 확보하는 데에도 이바지 할 것으로 기대된다.

• Nuclear Engineering and Technology
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• 제55권12호
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• pp.4491-4503
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• 2023

This study aimed to verify and validate the transient simulation capability of the hybrid code system RAST-F for fast reactor analysis. For this purpose, control rod (CR) drop experiments involving eight separate CRs and six CR groups in the China Experimental Fast Reactor (CEFR) start-up tests were utilized to simulate the CR drop transient. The RAST-F numerical solution, including the neutron population, time-dependent reactivity, and CR worth, was compared against the measurement values obtained from two out-of-core detectors. Moreover, the time-dependent reactivity and CR worth from RAST-F were verified against the results obtained by the Monte Carlo code Serpent using continuous energy nuclear data. A code-to-code comparison between Serpent and RAST-F showed good agreement in terms of time-dependent reactivity and CR worth. The discrepancy was less than 160 pcm for reactivity and less than 110 pcm for CR worth. RAST-F solution was almost identical to the measurement data in terms of neutron population and reactivity. All the calculated CR worth results agreed with experimental results within two standard deviations of experimental uncertainty for all CRs and CR groups. This work demonstrates that the RAST-F code system can be a potential tool for analyzing time-dependent phenomena in fast reactors.

• Nuclear Engineering and Technology
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• 제50권7호
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• pp.1024-1036
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• 2018

In this paper, McCARD code was verified using various models listed in the NUREG/CR-6361 benchmark guide, which provides specifications for single pin-cells, single assemblies, and the whole core classified depending on the nuclear properties and structural characteristics. McCARD code was verified by comparing its results with those of SCALE code for single pin-cell and single assembly benchmark problems. The difference in the multiplication factor obtained through the two codes did not exceed 90 pcm. The benchmark guide treats a total of 173 whole core experiments. The experiments are categorized as simple lattices, separator plates, reflecting walls, reflecting walls and separator plates, burnable absorber fuel rods, water holes, poison rods, and borated moderator. As a result of numerical simulation using McCARD, the mean value of the multiplication factors is 1.00223 and the standard deviation of the multiplication factors is 285 pcm. The difference between the multiplication factors and the experimental value is in the range of -665 pcm to + 1609 pcm. In addition, statistics of results for experiments categorized by reactor shape, additional structure, burnable poison, etc., are detailed in the main text.

• Nuclear Engineering and Technology
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• 제54권10호
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• pp.3604-3613
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• 2022

The Physical Protection System (PPS) plays an important role and must effectively deal with various adversary attacks in nuclear security. In specific single adversary path scenarios, we can calculate the PPS effectiveness by EASI (Estimated Adversary Sequence Interruption) through Probability of Interruption (P_I) calculation. EASI uses a single value of the probability of detection (P_D) and the probability of alarm communications (P_C) in the PPS. In this study, we develop a multi-path analysis code based on EASI to evaluate the effectiveness of PPS. Our quantification method for P_I considers the variability and uncertainty of P_D and P_C value by Monte Carlo simulation. We converted the 2-D scheme of the nuclear facility into an Adversary Sequence Diagram (ASD). We used ASD to find the adversary path with the lowest probability of interruption as the most vulnerable paths (MVP). We examined a hypothetical facility (Hypothetical National Nuclear Research Facility - HNNRF) to confirm our code compared with EASI. The results show that implementing the variability extension can estimate the P_I value and its associated uncertainty. The multi-path analysis code allows the analyst to make it easier to assess PPS with more extensive facilities with more complex adversary paths. However, the variability of the P_D value in each protection element allows a significant decrease in the PI value. The possibility of this decrease needs to be an important concern for PPS designers to determine the P_D value correctly or set a higher standard for PPS performance that remains reliable.

• 한국의학물리학회지:의학물리
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• 제22권4호
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• pp.190-197
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• 2011

고선량률 근접치료에 사용되는 상업용 선원과 치료계획 시스템들은 AAPM TG 43에서 권고하는 점 및 선 선원에 의해 선량분포를 계산한다. 하지만, 근접치료용 선원에 대한 인체 내의 정확한 선량계산을 위해서 3차원 부피의 선원을 고려하는 MC 기반의 선량계산 방법이 필요하다. 본 연구에서는 microSelectron HDR Ir-192 선원을 작은 부분으로 분할하여 계산하는 미소선원 적분법을 이용하여 기하학적 인수를 계산하였다. 또한, 범용 방사선 수송코드인 MCNPX를 사용하여 30 cm 직경의 구형 물 팬텀 내에서 선원의 선량률을 계산하여 비등방성함수와 반경선량함수를 구하였다. 그 결과를 MC 기반 광자 수송코드인 MCPT를 사용하여 계산한 Williamson의 결과와 비교 및 분석하였다. 미소선원 적분법과 선 선원 근사법에 따른 기하학적 인수는 $r{\geq}0.5cm$에서는 0.2% 이내에서 일치하였고 r=0.1 cm일 때 1.33%의 차이를 보였다. 본 연구에서 계산된 비등방성함수와 반경선량함수가 Williamson의 계산된 결과의 차이는 비등방성함수의 경우 r=0.25 cm에 서 2.33%의 가장 큰 R-RMSE를 보였고 $r{\geq}0.5cm$에서는 1% 미만의 R-RMSE를 보였다. 반경선량함수의 경우는 r=0.1~14.0 cm에서 0.46%의 R-RMSE를 보였다. 미소선원 적분법과 선 선원 근사법으로 계산한 기하학적 인수는 $r{\geq}0.1cm$에서 잘 일치하지만 3차원의 Ir-192 선원을 적용하여 계산한 미소선원 적분법이 실제 기하학적 인수를 잘 반영할 것으로 생각된다. r=0.25 cm에서 비등방성함수를 제외하고는 MCPT와 MCNPX의 몬테칼로 코드를 이용하여 얻어진 비등방성함수와 반경선량함수는 각각의 몬테칼로 코드에 대한 불확실성 이내에서 잘 일치함을 확인하였다. 따라서 MCNPX 전산모사 결과를 통해 TG-43의 선량 계산식에 사용된 인자를 Williamson 등의 결과와 비교 및 검증함으로써, 추후 다른 종류의 선원에 대해서도 Monte Carlo 기반의 연구가 가능할 것으로 기대된다.