• 전기학회논문지
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• 제60권4호
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• pp.694-699
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• 2011

This paper compares the performance of lightning shielding analysis methods using the seven striking distance formulae in substation. For comparison, we evaluate the number of expected strikes and exposed area using WinIGS Software. Seven striking distance formulae are compared using the electrogeometric model analysis and the rolling sphere method. Based on the electrogeometric model analysis, the risk of shielding failure in either the whole substation or parts of it is determined. According to the simulation results, one can justify whether the substation satisfies the criterion of shielding design. In particular, according to the rolling sphere method, the exposed areas in substation determine the location of the additional shielding poles or shield wires. Therefore, the installation of the additional shielding poles and shield wires in substation was accepted by shield design at the phase conductors exposed in the larger area.

• 한국초전도ㆍ저온공학회논문지
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• 제17권1호
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• pp.40-43
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• 2015

Wireless power transfer technology is using the magnetic resonance recently drawing increased attention. It uses the resonance between transmitter and receiver coils to transfer power. Thus, it can improve the transfer distance and efficiency compared with the existing magnetic induction technique. The authors found from the previous study that the application of the superconductor coil to the magnetic resonance wireless power transfer system improved its efficiency. Its application to real life, however, requires the additional study on the effects of adjacent materials. In this study, the two resonance coils made by superconductor coils were used to aluminum and plastic shielding materials was placed between the coils. S-parameters were analyzed according to the position of the shielding material between the transmitter and receiver coils. As a result, the plastic of shielding material had no effect, but the aluminum of shielding material affected the wireless power transfer due to the shielding effectiveness.

• 한국방사선학회논문지
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• 제17권6호
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• pp.889-896
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• 2023

핵의학과에서 가장 많이 사용되는 ^99mTc를 점선원과 산란팬텀을 이용하여 에너지스펙트럼 변화를 분석하고 변화된 감마선 에너지에 따른 납 앞치마의 차폐효과를 평가하였다. 산란팬텀의 감마선 에너지 스펙트럼은 점선원보다 광전피크 영역은 감소하고 컴프턴 산란영역은 증가하였다. 감마선원 형태 변화에 따른 에너지 영역별 계수치는 점선원의 계수치보다 20 cm 거리에서 최대 66.1 %의 감소율을 보였으며 컴프턴 산란 영역에서는 산란팬텀의의 계수치가 점선원의 계수치보다 최대 40 cm 거리에서 122.2 % 증가하는 결과를 보였다. 감마카메라를 이용한 선원과 산란팬텀의 거리에 따른 차폐율 차이에서 광전피크 영역은 유사한 결과를 보였으나 컴프턴 산란영역에서는 20 cm거리에서 산란팬텀의 차폐율이 점선원의 차폐율보다 29.2% 증가하였으며 거리가 증가함에 따라 차폐율 차이는 감소하였다. 방사선 선량계를 이용한 납 앞치마 차폐율 측정에서 산란팬텀의 차폐율은 최대 15.3 %의 차이를 보였으며 거리가 증가할수록 두 선원의 차폐율 차이는 감소하였다. 산란팬텀의 납 앞치마 차폐율이 점선원보다 높고 선원과 가까운 거리일수록 납 앞치마의 효과는 증가하는 결과로 방사성의약품을 주입한 환자를 직접 대면할 때 납 앞치마의 착용은 방사선피폭 저감화에 도움이 될 것으로 판단된다.

• Journal of Advanced Marine Engineering and Technology
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• 제36권2호
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• pp.294-301
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• 2012

지구온난화의 주원인으로서 $CO_2$가스 사용량 증가에 의한 온실효과가 전 세계적인 문제가 되고 있다. 특히, 조선산업 분야에서는 아크용접 시 보호가스로서 막대한 양의 $CO_2$가스가 사용되고 있기 때문에 $CO_2$가스 사용량을 감소시킬 수 있는 용접장비의 개발에 대한 요구가 커지고 있다. 따라서, 본 연구에서는 $CO_2$ 보호가스 사용량을 감소시킬 수 있는 토치노즐의 최적형상 설계인자를 검토하기 위한 기초연구로서 Tandem 용접기 토치 극간거리에 따른 $CO_2$ 보호가스 분포에 대해서 CFD해석을 수행하였으며, 극간거리와 아크전류 공급량에 따른 용접성에 대해서도 실험적으로 검토하였다. 토치간 거리에 따라서 가장 효과적인 보호가스층이 존재하며, 최적의 극간거리를 정량적으로 결정함에 의해 $CO_2$ 보호가스의 적정한 사용에 의한 $CO_2$ 가스 사용량을 감소시킬 수 있다.

• 대한방사선기술학회지:방사선기술과학
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• 제41권2호
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• pp.135-140
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• 2018

In this study, the dose of antimony shielding sheet was measured and the shielding rates according to the distance between the radioisotopes and the detector was analyzed according to the type of $^{99m}Tc$, $^{18}F$, $^{201}Tl$, $^{131}I$, $^{123}I$ using the antimony shielding sheet. The detector was used with an inspector. Six sheets of 0.25 mmPb were prepared with 20 cm width and length. Measurement results using $^{99m}Tc$, $^{201}Tl$, and $^{123}I$ showed that as the thickness of the sheet became thicker, the farther the distance from the source to the sheet was, the smaller the transmitted dose amount was measured. It was analyzed that a thickness of 1.50 mm or more was required to obtain a shielding rates of 90% or more. In the experiments of $^{18}F$ and $^{131}I$, the dose value was highest when 0.25 mm sheet was used, and the shielding rates was negative, unlike the results of other radioisotopes. Since $^{201}Tl$ are used when using antimony sheet and $^{18}F$ and $^{131}I$ have no shielding effect, it is thought that it is effective to reduce dose by repeating training and simulation training so that work can be done in a short time.

• 한국산학기술학회논문지
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• 제19권9호
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• pp.124-129
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• 2018

본 연구는 Apron의 재질로 이용되고 있는 텅스텐 차폐체를 핵의학과에서 사용하는 선원의 종류와 차폐체의 두께, 선원부터 검출기 사이의 거리를 변화시켜 차폐체에 투과시킨 후 투과선량과 차폐율을 알아보고자 하였다. 실험을 위해서 선원과 차폐체와 검출기를 일직선으로 배치하고 높이 100 cm 지점에서 Inspector로 측정하였다. 그 결과 텅스텐에 차폐효과가 가장 높은 선원은 $^{201}Tl$ 선원으로 측정되었고, $^{123}I$ 선원이 $^{99m}Tc$ 선원보다 차폐효과가 높게 나타났다. 실험에 사용한 선원과 검출기 사이의 거리는 멀어질수록 투과선량은 작아졌고, 텅스텐 차폐체의 두께는 두꺼울수록 차폐율은 높게 측정되었다. 하지만 $^{131}I$와 $^{18}F$ 선원에서는 0.25 mmPb의 차폐체를 사용했을 경우 차폐체가 없을 경우 보다 차폐율이 감소하는 것을 확인하였다. 따라서 $^{13}1I$와 $^{18}F$ 선원을 사용할 경우에는 방사선 차폐효과가 높은 텅스텐일지라도 선원의 종류에 따른 특성과 차폐체의 두께를 고려하여 사용하길 권장하고, 실험 결과를 참고하여 사용한다면 피폭 저 감화방안에 도움을 줄 수 있을 것으로 생각된다.

• Journal of Welding and Joining
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• 제34권5호
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• pp.6-12
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• 2016

This study was performed bead welding of pure titanium by using fiber laser. Since titanium is very sensitive to oxidation and nitriding during welding, it is important to compose the shielding equipment compared with different material. Thus side and coaxial shield nozzle, rail and chamber type shielding equipment are widely used to protect effectively the weld during welding. Experiments were performed by changing nozzle angle and distance using side and coaxial shield nozzle. The bead colors of gold, brown, blue, purple and yellowish white were obtained by changing variables of shield nozzle, and then its weldability was investigated. As experiment result, sound and not brominated beads were formed when side nozzle angle and distance were respectively $45^{\circ}$ and 10 mm.

• Progress in Superconductivity
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• 제11권1호
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• pp.30-35
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• 2009

We have investigated the characteristics of a superconductive Pb shield for hemispherical shape and plate to improving signal-to-noise ratio(SNR) of biomagnetism. We measured the shielding factor for the position of helmet shape Pb and for changing the distance from Pb surface. To make a uniform magnetic field, a $1.5m{\times}1.5m$ set of the helmholtz coils activated at several frequencies. The shielding factor of hemispherical shape Pb was from 20 to 57 dB and of Pb plate was about $6{\sim}26dB$ as a function of distance from the lead surface. The shielding factor was rapidly reduced as increasing the distance from Pb surface. The white noise of superconductive quantum interference device(SQUID) with a superconductive shield was about $12fT/Hz^{1/2}$ at 1 Hz, $7fT/Hz^{1/2}$ at 100 Hz. The white noise was more increased about two times than conventional SQUID system without Pb shielding. An auditory signal was measured by first order gradiometer and magnetometer with Pb superconductive shield and compared the SNR. The SQUID system with Pb shield had better performance at low frequency noise level.

• 대한방사선기술학회지:방사선기술과학
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• 제42권5호
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• pp.373-377
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• 2019

Radiation exposure is on the rise as the working hours of radiation workers increase. Accordingly, the importance of protection products for decreasing the dose of exposure has risen, and excellent X-ray shielding ability and light weight are required. The purpose of this study is to compare the Pb which use currently and other elements in order to reduce the exposure of workers to the most effective protection products. For experiment, we used the general X-ray equipment and angiography equipment, and obtained the Pb and apron's shielding rate. When the shielding rate of Pb and apron was compared in general X-ray equipment, the shielding rate was 95.1% for Pb 0.5 mm, 96.1% for apron 0.5 mmPb and 95.6% for Bi+W 0.5 mmPb. When compared the shielding rate of each aprons in angiography equipment, 0.5 mmPb apron was the highest as 96.4% and Bi+W 0.25 mmPb apron was the lowest as 90.2% at the 50 cm distance. The shielding rate of 0.5 mmPb apron was the highest as 95.7% and Bi+W 0.25 mmPb apron was the lowest as 85.9% at the 100 cm distance. As a result of evaluating the apron efficiency through this study, 0.5 mmPb apron showed the best shielding rate, but it was the heaviest apron. 0.35 mmPb apron and Bi+W 0.25 mmPb apron weighed light but had low shielding rate. Through the results of this experiment, it is recommended that radiation workers reduce radiation exposure by using more efficient protection products.

• 한국융합학회논문지
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• 제9권7호
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• pp.87-93
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• 2018

본 연구는 핵의학과에서 많이 사용하고 있는 $^{99m}Tc$, $^{123}I$, $^{201}Tl$, $^{18}F$, $^{13}1I$를 비스무트 차폐체에 투과시킨 후 방사성동위원소의 종류와 측정 거리변화에 따라 차폐율을 알아보고자 하였다. 실험을 위해 납당량 0.25 mmPb, 비스무트 차폐체 6장을 두께가 두꺼워 질수록 1.50 mm까지 한 장씩 겹쳐 사용하였고, 거리를 30 cm, 50 cm, 100 cm로 두고 투과선량을 측정하였다. 그 결과 두께가 두꺼워질수록 차폐율이 높게 측정되었고 거리를 멀리할수록 측정값은 작아졌다. $^{99m}Tc$보다 $^{123}I$와 $^{201}Tl$의 차폐율이 가장 높게 나타나 차폐효과가 우수한 것을 확인하였고, $^{18}F$와 $^{131}I$는 고에너지와 ${\beta}$선으로 인해 차폐체가 없을때보다 차폐체가 있을때 차폐효과가 떨어지는 것으로 나타났다. 실험결과를 참고하여 방사성동위원소의 종류에 따라 비스무트 차폐체를 사용한다면 핵의학 종사자들의 피폭 저감화와 피폭관리 방안에 도움을 줄 수 있을 것으로 생각된다.