• Title/Summary/Keyword: 빔 차폐

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Correction of Radar Reflectivity over Beam Blocking Area by Accumulated Radar Reflectivity (레이더 반사도 누적 방법을 이용한 지형에 의한 부분차폐영역의 레이더 반사도 보정)

  • Park, Sung-Hwan;Jung, Sung-Hwa;Lee, Jung-Hoon;Kim, Kyeong-Eak
    • Journal of Korea Water Resources Association
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    • v.42 no.8
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    • pp.607-617
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    • 2009
  • Radar beam blocking which is partially or entirely interrupted by obstacles like a mountain causes underestimation of the rainfall. In this paper, partially blocked radar reflectivity is retrieved using the ARM(Accumulated Reflectivity Map). ARM is made by accumulation of the radar reflectivity and very useful product to analyze the beam blockage. The blockage correcting map could be obtained by assuming the spatially uniform reflectivity field in the ARM. This method is applied to the cases of typhoon and Changma, and we obtain the MFE(Mean Fractional Error) from two radar data, the one is objective radar data which is affected by blockage and the other is comparative radar data which is not affected by blockage. Before blocking correction, MFE is 20-35%. However, after correction, MFE decreases to 7-10%.

Calculation Formula for Shielding Thickness of Direct Shielded Door installed in Treatment Room using a 6 MV X-ray Beam (6 MV X-선 빔을 사용하는 치료실에 설치되는 직접 차폐식 도어의 차폐 두께 계산식)

  • Park, Cheol Seo;Kim, Jong Eon;Kang, Eun Bo
    • Journal of the Korean Society of Radiology
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    • v.14 no.5
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    • pp.545-552
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    • 2020
  • The purpose of this study is to derive a lead thickness calculation formula for direct-shielded doors based on NCRP Report No.151 and IAEA Safety Report Series N0.47. After deriving the dose rate calculation formula for the direct shielded door, this formula was substituted for the lead shielding thickness calculation formula to derive the shielding thickness calculation formula at the door. The lead shielding thickness calculated from the derived direct shielded door shielding thickness calculation formula was about 6% lower than that calculated by the NCRP and IAEA secondary barrier shielding thickness calculation methods. This result is interpreted as meaning that the thickness calculation is more conservative from the NCRP and IAEA secondary barrier shielding thickness calculation methods and fits well for secondary beam shielding. In conclusion, it is thought that the formula for calculating lead shielding thickness of the direct shielded door derived in this study can be usefully used in the shield design of the door.

Shielding Design Optimization of the HANARO Cold Neutron Triple-Axis Spectrometer and Radiation Dose Measurement (냉중성자 삼축분광장치의 차폐능 최적화 설계 및 선량 측정)

  • Ryu, Ji Myung;Hong, Kwang Pyo;Park, J.M. Sungil;Choi, Young Hyeon;Lee, Kye Hong
    • Journal of Radiation Protection and Research
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    • v.39 no.1
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    • pp.21-29
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    • 2014
  • A new cold neutron triple-axis spectrometer (Cold-TAS) was recently constructed at the 30 MWth research reactor, HANARO. The spectrometer, which is composed of neutron optical components and radiation shield, required a redesign of the segmented monochromator shield due to the lack of adequate support of its weight. To shed some weight, lowering the height of the segmented shield was suggested while adding more radiation shield to the top cover of the monochromator chamber. To investigate the radiological effect of such change, we performed MCNPX simulations of a few different configurations of the Cold-TAS monochromator shield and obtained neutron and photon intensities at 5 reference points just outside the shield. Reducing the 35% of the height of the segmented shield and locating lead 10 cm from the bottom of the top cover made of polyethylene was shown to perform just as well as the original configuration as radiation shield excepting gamma flux at two points. Using gamma map by MCNPX, it was checked that is distribution of gamma. Increased flux had direction to the top and it had longer distance from top of segmented shield. However, because of reducing the 35% of the height, height of dissipated gamma was lower than original geometry. Reducing the 35% of the height of the segmented shield and locating lead 10cm from the bottom of the top cover was selected. After changing geometry, radiation dose was measured by TLD for confirming tester's safety at any condition. Neutron(0.21 ${\mu}Svhr^{-1}$) and gamma(3.69 ${\mu}Svhr^{-1}$) radiation dose were satisfied standard(6.25 ${\mu}Svhr^{-1}$).

Evaluation of the Usefulness of Tungsten Nanoparticles as an Alternative to Lead Shielding Materials in Electron Beam Therapy (전자선 치료시 납 차폐체 대체물질로서의 텅스텐 나노입자의 유용성 평가)

  • Kim, Ji-Hyang;Kim, Na-Kyoung;Lee, Gyu-Yeong;Jung, Da-Bin;Heo, Yeong-Cheol
    • Journal of the Korean Society of Radiology
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    • v.15 no.7
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    • pp.949-956
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    • 2021
  • The purpose of this paper is to evaluate whether tungsten nanoparticles have a shielding effect on scattered light generated at high doses as an alternative material to lead used to shield scattered light in electron beam therapy. A plate was manufactured to set the position of the dosimeter and the size of the radiation field to be constant. The glass dosimeter was placed at 12 points, which were 1, 2, and 4 cm apart from the center of the field of 10 × 10 cm2 in the cross direction. A total of 12 types of tungsten nanoparticle shields were developed with a thickness of 0.75 mm to 4.00 mm and a size of 10 × 10 cm2 using 0.4, 0.75, and 1 mm materials. Using a linear accelerator, measurements were made four times at 6 MeV and four times at 12 MeV, and the dose intensity was investigated at 100 MU. The 4 mm shielding plate showed the highest shielding effect at 1 cm from the irradiation field. The 1 mm shielding plate at 2 cm from the irradiation field had the lowest shielding effect. As the thickness of the tungsten shielding plate increased, the electron beam's shielding effect increased sharply. It was confirmed that tungsten nanoparticles can reduce the amount of scattered light generated by electron beam therapy. Therefore, this study will provide basic data when follow-up studies are conducted on the shielding ability of tungsten nanoparticles.

400 MeV/nucleon 12C Ions Shielding Benchmark Calculations using MCNPX with Different Nuclear Data Libraries (400 MeV/nucleon 12C 이온의 MCNPX 와 핵자료를 이용한 차폐 벤치마킹 계산)

  • Shin, Yun Sung;Kim, yong min;Kim, dong hyun;Jung, nam suk;Lee, hee seock
    • Journal of the Korean Society of Radiology
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    • v.9 no.5
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    • pp.295-300
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    • 2015
  • There are various type of particle accelerators such as Kyoungju 100-MeV proton beam accelerator in Korea. And Korea plans to build large particle accelerator such as heavy ion accelerator and 4th generation light source facility. The accelerated high energy particles of these facility produce 2nd neutron after nuclear reaction with target materials. And then these 2nd neutron activate structural materials and surrounding environment. Accordingly, it is important to consider the activation and shielding calculation on design of facility for safety operation. In this study, we tried to calculate and compare the neutron flux from the interaction $^{la}150$ beam with target material(Cu) according to thickness of iron and concrete shielding material by MCNPX 2.7 with nuclear library JENDL/HE 07and la150. To verify the properties of nuclear library, we compared computational results with experimental value. These results can be used for dose evaluation technology in planning of the shielding of large particle accelerator.

Retrieval of Damaged Weather Radar Data using Image Morphology Technique (영상 모폴로지 기법을 활용한 손상된 기상레이더자료 보정 기법)

  • Jang, Kong-Joo;Kim, Hyunjung;Lim, Sanghun;Lee, Keon-Haeng;Hyun, Myung-Suk;Lee, Dong-Ryul
    • Proceedings of the Korea Water Resources Association Conference
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    • 2016.05a
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    • pp.19-19
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    • 2016
  • 오늘날, 보다 정밀한 대기기상 분석과 정확한 기상 예측을 위해 보편적으로 기상레이더를 활용하고 있다. 지표면과 가까운 저층에서 주로 발생하는 국지성 호우 및 돌발기상에 대한 대응을 위해서는 기상레이더 역시 저층 관측이 수반되어야 한다. 하지만, 국토 대부분이 산악지형으로 이루어진 우리나라에서는 산악지형에 의한 지형클러터와 빔 차폐의 영향을 피하여 원만한 기상관측을 위해 대부분의 기상레이더가 고지대에 설치, 운영되고 있다. 그럼에도 불구하고 낮은 고도각의 레이더 관측 자료에서는 여전히 지형 클러터 및 차폐에 따른 영향으로 인해 자료 품질의 신뢰성이 떨어질 수 밖에 없다. 현재 클러터나 차폐가 발생한 영역에 대해 상위 고도각의 자료를 이용하는 등의 방법으로 보정을 수행하고 있지만 각 고도각 관측 자료들의 시간적 차이가 발생함에 따라 부정확성이 발생할 수 있다는 단점이 있다. 따라서 본 논문에서는 차폐 영역 보정에 대한 처리를 위해 단일 관측자료 만을 이용하는 방법을 적용함으로서 시간적 불일치성에 대한 문제를 해결하고, 초단기 강수예측을 위한 강수에코의 정확한 추적을 위해 레이더 영상에 적응적인 차폐, 클러터 보정 기법을 제안한다. 제안 기법은 강수에코의 형태학적 구조에 기반한 차폐보정을 위해 영상 처리 기법의 한 종류인 모폴로지 기법을 적용함으로써 강수에코의 모양, 크기, 및 구조에 따라 침식 및 팽창 과정을 수행하여 클러터나 차폐로 인해 소실된 강수에코 영역을 보정한다. 실험결과 레이더 강수추정의 정확성 향상을 꾀할 수 있었으며, 강수 추적을 위한 강수에코의 형태학적 복원이 가능함을 확인하였다. 이로부터, 향후 저층관측 레이더 자료의 활용성 증대와 에코 형태에 기반한 강수 추적 알고리즘 개발 및 성능 향상에 활용될 수 있을 것으로 기대한다.

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Characteristics of Dose Distribution at Junctional Area Using the Divergency Cutout Block in the Abutted Field of Photon and Electron Beams (광자선과 전자선의 인접조사에서 선속 퍼짐현상이 고려된 전자선 차폐물을 이용한 접합 조사면의 선량분포 특성)

  • Im, In-Chul;Lee, Jae-Seung
    • Journal of Radiation Protection and Research
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    • v.36 no.3
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    • pp.168-173
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    • 2011
  • This study investigated characteristics of dose distribution at junction field of X-ray and electron beams according to the method for fabricating the insert block on the electron cone. Insert block were fabricated to the divergency cutout block and the straight cutout block. For the 6 MV X-ray and 10 MeV nominal energy of electron beam, we was adjacent to the light field of X-ray and electron beam at a surface of matrix chamber and measured to beam profile of abutted field in the 0, 1, 2, 3 cm measurement depth. As a result, characteristics of dose distribution at junction field, straight block was existent that over dose area exceed the give dose more than 5% and under dose area with a rapid change in dose distribution. However, divergency block had remarkably decreased the over dose area caused by the lateral scattering effects of decrease, and being existed uniformity dose distribution in the junction field. Therefore, divergency block were the benefits of radiation dose delivery, in order to applied the clinical, measurement of electron beams according to the fabrication method of the block should be considered carefully.

Simulation of Radar Network for Observational Gap Filling as Electromagnetic Waves Beam Blockage in the Korean Peninsula (전자기파 빔 차폐 사각 지역 해소를 위한 한반도 레이더 관측망 모의)

  • Jo, Jun-Mo;Kwon, Byung-Hyuk;Yoon, Hong-Joo
    • The Journal of the Korea institute of electronic communication sciences
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    • v.15 no.3
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    • pp.553-562
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    • 2020
  • S-band, C-band and X-band radars are used for weather observation purposes. Since the Meteorological Administration, the Ministry of Environment, and Republic of Korea Air Force operate radars according to the purpose of observation by departments, the installation site and observation characteristics are different. From a meteorological point of view, blind observational areas in the low level with an elevation of less than 1 km around the mountainous terrain near Jirisan and Taebaeksan. Assuming a small radar installation, we simulated low-level observations. In order to monitor dangerous weather in North Korea, we analyzed the precipitation of North Korea and simulated a large radar network. Finally, a radar network for Korean Peninsula was proposed.

Channel Interference Analysis of Wideband WLAN Based IEEE802.11n for 3rd Generation Digital Signage (3세대 디지털 사이니지를 위한 IEEE802.11n 광대역 무선랜에 대한 채널 간섭 분석)

  • Ko, Hojeong
    • Journal of Satellite, Information and Communications
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    • v.11 no.1
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    • pp.6-11
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    • 2016
  • In this paper, we have analyzed the effects of co-channel, adjacent-channel, and the human shield(Body Blockage) for wideband WLAN based on the IEEE802.11n 40MHz channel bandwidth required for high speed digital signage service. Simulation results show that wideband WLAN can be operated with 78 interferers over 63m distance in co- channel, 80 interferer over 61m distance in adjacent channel. By applying the mitigation method for reducing the interference, we have confirmed that protection distance is improved to 51m using beamforming, and 40m using cognitive radio in co-channel interference. Also body blockage interference is reduced using adaptive channel bandwidth, C/I ratio, beamforming, power control mitigation methodology.