비유사량(沸流砂量) 추정방법의 개발(I) -개발방향의 설정 및 자료의 수집·분석 -

유권규,김창완,김형섭,우효섭,Yu, Kwon Kyu,Kim, Chang Wan,Kim, Hyoung Seop,Woo, Hyo Seop 대한토목학회 1993 대한토목학회논문집 Vol.13 No.1

The major objective of this study is to develop practical methods for estimating sediment yield rates of medium size watersheds of which areas range from 200 to $2,000km^2$. For this purpose, this study adopts an empirical method of statistical approach and another empirical method of weighting the watershed characteristics factors. A total of 13 data points for sediment yield rate, including five data points from reservoir deposit data and eight data points from sampled river-sediment data have been collected. Meanwhile, seven factors that may affect the sediment yield rate of a watershed have been selected. They are drainage density, rainfall erosivity, ground cover and land use, soil erodibility, topography, river-bed material characteristics, and watershed area. In the companion paper following this paper, methods for estimating sediment yield rate are to be developed using the 13 data points collected and seven watershed characteristics factors selected in this study. 본 연구의 주요 목적은 댐 설계를 위한 유역의 비유사량 추정방법을 개발하는 것으로 유역면적 $200km^2{\sim}2,000km^2$ 정도의 중규모 유역을 대상으로 한다. 이를 위하여, 본 연구에서 개발할 비유사량 추정방법으로 통계적 방법에 의한 경험식과 미국 PSIAC 방법과 유사한 도표식 방법을 채택하였다. 이러한 방법들의 개발을 위해 본 연구에서는 과거 '60년대 이후 우리나라에서 수행된 하천유사량 실측자료 및 기존 다목적 및 발전댐 저수지 퇴사자료를 모두 수집 분석하여 비유사량 추정방법의 개발에 이용 가능한 자료 5 점을 도출하였다. 또한, 섬강, 금강상류, 내성천, 위천 등 4 개 조사유역의 8개 지점에서 하천유사량 자료를 실측하여 8개 지점에서의 연평균 비유사량을 산정하였다. 한편, 유역의 비유사량에 영향을 주는 유역특성 인자로 유역면적, 하천밀도, 강우 침식도, 식생 및 토지이용, 토양 침식성, 지형(기복 에너지), 하상재료 당 총 7 개의 유역특성인자를 선정하고, 각 인자의 정량화 방법을 제시하였다. 연구(II)에서는 이러한 유역특성 인자들과 중규모 유역에서 수집된 13 점의 이용가능한 유역 비유사량 자료를 이용하여 비유사량 추정방법을 개발한다.

권선형 1차 미분계를 이용한 태아심자도 신호 측정

유권규,김기웅,강찬석,김진목,이용호,Yu, K.K.,Kim, K.,Kang, C.S.,Kim, J.M.,Lee, Y.H. 한국초전도학회 2009 Progress in superconductivity Vol.10 No.2

We have fabricated a low-noise 61-channel axial-type first-order gradiometer system for measuring fetal magnetocardiography(MCG) signals. Superconducting quantum interference device(SQUID) sensor was based on double relaxation oscillation SQUID(DROS) for detecting biomagnetic signal, such as MCG, magnetoencphalogram(MEG) and fetal-MCG. The SQUID sensor detected axial component of fetal MCG signal. The pickup coil of SQUID sensor was wound with 120 ${\mu}m$ NbTi wire on bobbin(20 mm diameter) and was a first-order gradiometer to reject the environment noise. The sensors have low white noise of 3 $fT/Hz^{1/2}$ at 100 Hz on average. The fetal MCG was measured from $24{\sim}36$ weeks fetus in a magnetically shielded room(MSR) with shielding factor of 35 dB at 0.1 Hz and 80 dB at 100 Hz(comparatively mild shielding). The MCG signal contained maternal and fetal MCG. Fetal MCG could be distinguished relatively easily from maternal MCG by using independent component analysis(ICA) filter. In addition, we could observe T peak as well as QRS wave, respectively. It will be useful in detecting fetal cardiac diseases.

파키스탄 여행기

유권규 대한토목학회 1993 대한토목학회지 Vol.41 No.2

진공조에 위치한 1차 SQUID 미분계를 이용한 헬멧형 뇌자도 장치의 제작

유권규,김기웅,이용호,Yu, K.K.,Kim, K.,Lee, Y.H.,Kim, J.M. 한국초전도학회 2009 Progress in superconductivity Vol.11 No.1

We have fabricated a helmet type magnetoencephalogrphy(MEG) with a $1^{st}$ order gradiometer in vacuum to improve the signal-to-noise ratio(SNR) and the boil-off rate of liquid helium(LHe). The axial type first-order gradiometer was fabricated with a double relaxation oscillation SQUID(DROS) sensor which was directly connected with a pickup coil. The neck space of LHe dewar was made to be smaller than that of a conventional dewar, but the LHe boil-off ratio appeared to increase. To reduce the temperature of low Tc SQUID sensor and pickup coil to 9 K, a metal shield made of, such as copper, brass or aluminum, have been usually used for thermal transmission. But the metal shield exhibited high thermal noise and eddy current fluctuation. We quantified the thermal noise and the eddy current fluctuation of metal. In this experiment, we used the bobbin which was made of an alumina to wind Nb superconductive wire for pickup coil and the average noise of coil-in-vacuum type MEG system was $3.5fT/Hz^{1/2}$. Finally, we measured the auditory evoked signal to prove the reliability of coil-in-vacuum type MEG system.

헬멧형 뇌자도 장치로의 활용을 위한 Pb 초전도 차폐의 특성

유권규,김기웅,이용호,Yu, K.K.,Kim, K.,Lee, Y.H.,Kwon, H. 한국초전도학회 2009 Progress in superconductivity Vol.11 No.1

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.

일본의 長良川 하구둑을 둘러싼 논쟁

유권규 대한토목학회 1995 대한토목학회지 Vol.43 No.10

ZnO : Al 투명도전막의 열처리특성에 대한 연구 ( A Study on the Heat Treatment Effects of ZnO : Al Transparent Conductive Thin Films )

유권규,홍천일,김정규,이형기,전춘배,박기철 대한전자공학회 1998 대한전자공학회 학술대회 Vol.1998 No.7

고감도 SQUID 냉각을 위한 저잡음 듀아의 설계 및 특성 조사

유권규,이용호,김기웅,권혁찬,김진목,Yu, K.K.,Lee, Y.H.,Kim, K.,Kwon, H.,Kim, J.M. 한국초전도학회 2010 Progress in superconductivity Vol.11 No.2

We have fabricated the low noise liquid helium(LHe) dewar with a different shape of thermal shield to apply the 64-channel SQUID(Superconducting Quantum Interference Device) gradiometer. The first shape of thermal shield was made of an aluminum plate with a wide width of 100 mm slit and the other shape was modified with a narrow width of 20 mm slit. The two types of dewars were estimated by comparing the thermal noise and the signal-to-noise ratio(SNR) of magnetocardiography(MCG) using the $1^{st}$ order SQUID gradiometer system cooled each dewar. The white noise was different as a point of the dewar. The noise was increased as close as the edge of dewar, and also increased at the thermal shield with the more wide width slit. The white noise of the dewar with thermal shield of 100 mm slit was 6.5 fT/$Hz^{1/2}$ at the center of dewar and 25 fT/$Hz^{1/2}$ at the edge, and the white noise of the other one was 3.5 - 7 fT/$Hz^{1/2}$. We measured the MCG using 64-channel SQUID gradiometer cooled at each LHe dewar and compared the SNR of MCG signal. The SNR was improved of 10 times at the LHe dewar with a modified thermal shield.

Parallel-loop 검출코일을 가지는 단일층 YBCO dc-SQUID 자력계의 제작 및 특성 연구

유권규,김인선,박용기 한국초전도학회 2003 Progress in superconductivity Vol.5 No.1

We have designed and fabricated the single-layer high $T_{c}$ SQUID magnetometer consisting of a directly coupled grain boundary junction SQUID with an inductance of 100 pH and 16 nested parallel pickup coils with the outermost dimension of 8.8 mm ${\times}$ 8.8 mm. The magnetometer was formed from a YBCO thin film deposited on an STO(100) bicrystal substrate with a misorientation angle of $30^{\circ}$. The SQUID magnetometer was further improved by optimizing the multi-loop pickup coil design for use in unshielded environments. Typical characteristics of the dc SQUID magnetometer had a modulation voltage of 40 $\mu\textrm{V}$ and a white noise of $30fT/Hz^{1}$2/. The SQUID magnetometer exhibited a 1/f noise level at 10 Hz reduced by a factor of about 3 compared with that of the conventional solid type pickup coil magnetometers and a very stable flux locked loop operation in magnetically disturbed environments.s.

충적하천(沖積河川)의 하상마찰(河床摩擦) 변화(變化)에 대한 조사(調査)·분석(分析)

유권규,김형섭,김활곤,우효섭,Yu, Kwon Kyu,Kim, Hyoung Seop,Kim, Hoal Gon,Woo, Hyo Seop 대한토목학회 1993 대한토목학회논문집 Vol.13 No.4

본 연구는 충적하천(沖積河川)에서 실측된 자료를 이용하여 한 하천지점에서 유량의 변화에 따른 하상형태의 변화와 그에 따른 하천마찰의 변화를 검토하는 것이다. 본 연구는 다음과 같은 조건의 하천상태에 국한한다: (1) 하폭 100m 내외의 중규모 하천, (2) 하천선형이 직선이고 하천단면의 변화가 적어 하상마찰 이외에 특별한 에너지 손실요인이 없는 하천, (3) 프루우드 수가 0.5 이하인 저수류영역(低水流領域) 하천. 본 연구에서 얻은 주요 결론을 요약하면 다음과 같다: (1) 매닝의 조도계수(粗度係數)는 평탄하상(平坦河床)의 경우 0.02정도에서 사구(砂丘) 형성시 0.05 정도로 2배 이상 증가한다. (2) 충적하천의 조도계수는 Strickler 공식 형태의 고정상 하천에 대한 조도계수 추정방법으로는 얻을 수 없다. (3) 기존의 하천시설기준에 수록된 이동상 하천에서의 조도계수 추정방법은 실제하천에 적용하는데 있어 한계가 있으며, 우리나라 자료를 이용한 구체적인 연구가 요망된다. Changes in bed forms and subsequent changes in channel roughness by changes in water discharge are discussed with the field data collected from some alluvial rivers in Korea. This study is limited to the following condition of river flow: (1) Medium size alluvial rivers with their widths of 100 m more or less, (2) Straight and prismatic river reach with no additional causes for energy loss but bed friction, (3) Lower-flow regime with Froude number less than 0.5. Major conclusions obtained from this study can be summarized as follows: (1) For the channels considered in this study, the bed roughness expressed by Manning's n increases from 0.02 for the plane beds with no sediment motion to 0.05 for the dune beds, (2) The roughness coefficient for alluvial channels should not be estimated from Strickler-type equations developed for the fixed beds, (3) The method for determining the channel roughness suggested in the present guideline for river works, River Structure Standard, appears to be lack of generality. More research based on the field data collected in Korea is needed in order to improve the existing methods.