• Title/Summary/Keyword: Multi-stacked

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대전류 통전을 위한 YBCO CC 적층선재의 자화손실 특성 (Characteristics of the Magnetization Loss in Stacked YBCO Coated Conductors for Large Current Application)

  • 이지광;임형우;차귀수
    • 한국초전도ㆍ저온공학회논문지
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    • 제9권1호
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    • pp.27-31
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    • 2007
  • For large power applications, multi-stacked tape should be used because single tape is limited in flowing demanded current capacity. Besides insulation between layers is needed for safe operation because high voltages are generated in those applications. In this study, considering those situations which mentioned above, we measure the magnetization loss in several multi-stacked tape samples having the different insulation thicknesses and various packing numbers of tape by external magnetic field having various incidence angles.

다중 스택 빔 형성을 이용한 고 지향성의 다중 목표물 고각 추정에 대한 연구 (A Study on Multi Target Elevation Angle Estimation of Hight Directivity using Multi Stacked Beam Forming)

  • 이관형;송우영;이명호
    • 한국컴퓨터정보학회논문지
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    • 제16권8호
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    • pp.129-135
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    • 2011
  • 본 논문에서는 다중 빔 형성기법을 이용하여 다중 목표물들의 고각을 추정하는 방법을 제안한다. 이 방법은 배열 소자로 수신되는 신호들을 디지털로 처리해 수신 빔을 스택 빔으로 만들고, 빔 형성기에서는 안테나 소자에 가중치를 적용함으로서 원하는 수신 빔을 생성 할 수 있다. 이때 스택 빔을 구현하기 위해서는 여러 개의 값비싼 위상천이기 필요하지만, 현재는 컴퓨터의 성능이 많이 향상되어 위상변위기 대신에 고속 푸리에 변환을 이용하여 다중스택 빔을 형성한다. 또한 수신기에서 원하는 방향으로 빔을 조향하기 위해서 빔 조향 오차 보정 기법을 적용하여 다중 빔의 지향성을 향상 시킨다. 본 논문에서는 시뮬레이션을 통하여 고속 후리어 변환과 빔 조향오차 보정 기법에 근거를 둔 제안된 고각 추정방법이 기존의 방법에 비해 목표물 추정 면에서 우수함을 보인다.

적층 수에 따른 YBCO 선재의 전송전류 손실 특성 (Characteristic of Transport Current Losses of Multi-Stacked YBCO Coated Conductors)

  • 한병욱;임희현;강명훈;임형우;차귀수;이희준
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2006년도 제37회 하계학술대회 논문집 D
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    • pp.2231-2232
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    • 2006
  • Multi-stacked HTS tapes are needed to conduct large current in the power application of superconducting machine. This paper deals with the transport current loss of multi-stacked YBCO coated conductor. YBCO coated conductor that was used in this experiment has two Cu layers above and below of YBCO layer for stabilization. Transport losses of four different stacks, single, 2 stack, 3 stack and 4 stack, were measured. Measured results were compared analytic equation suggested by Norris.

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적층 수에 따른 YBCO 선재의 전송전류 손실 특성 (Characteristic of Transport Current Losses of Multi-Stacked YBCO Coated Conductors)

  • 한병욱;임희현;강명훈;임형우;차귀수;이희준
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2006년도 제37회 하계학술대회 논문집 B
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    • pp.1265-1266
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    • 2006
  • Multi-stacked HTS tapes are needed to conduct large current in the power application of superconducting machine. This paper deals with the transport current loss of multi-stacked YBCO coated conductor. YBCO coated conductor that was used in this experiment has two Cu layers above and below of YBCO layer for stabilization. Transport losses of four different stacks, single, 2 stack, 3 stack and 4 stack, were measured. Measured results were compared analytic equation suggested by Norris.

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적층 수에 따른 YBCO 선재의 전송전류 손실 특성 (Characteristic of Transport Current Losses of Multi-Stacked YBCO Coated Conductors)

  • 한병욱;임희현;강명훈;임형우;차귀수;이희준
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2006년도 제37회 하계학술대회 논문집 C
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    • pp.1725-1726
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    • 2006
  • Multi-stacked HTS tapes are needed to conduct large current in the power application of superconducting machine. This paper deals with the transport current loss of multi-stacked YBCO coated conductor. YBCO coated conductor that was used in this experiment has two Cu layers above and below of YBCO layer for stabilization. Transport losses of four different stacks, single, 2 stack, 3 stack and 4 stack, were measured. Measured results were compared analytic equation suggested by Norris.

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1세대 선재와 2세대 선재의 혼합 적층에 따른 자화손실 특성 (Magnetization loss of Hybrid Multi-Stacked wire made of 1G wires and 2G wires)

  • 임형우;이용석;이희준;차귀수
    • 한국초전도ㆍ저온공학회논문지
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    • 제9권1호
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    • pp.57-60
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    • 2007
  • Superconducting electric power devices need to stack HTS wires to increase the current carrying capacity. Uniform multi-stacked wires(UMS) which were made of the same HTS wires have been used. This paper shows the magnetization loss of hybrid multi-stacked(HMS) wire made of BSCCO wires and YBCO wires. Five HMS wires, YB(YBCO-BSCCO), YYBB. YBYB, YBBY and BYYB, were made and tested. Magnetization losses of each UMS wire were compared with corresponding HMS wire. Test results show that magnetization losses per unit length of HMS wire are between the corresponding UMS BSCCO wire and HMS YBCO wire below critical magnetic field. Above the critical magnetic field, magnetization losses of HMS wires are larger than that of corresponding both VMS wires.

Analysis of Stacked and Multi-layer Graphene fot the Fabrication of LEDs

  • 김기영;민정홍;장소영;이준엽;박문도;김승환;전성란;송영호;이동선
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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    • pp.433.1-433.1
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    • 2014
  • The research of graphene, a monolayer of carbon atoms with honeycomb lattice structure, has explosively increased after appeared in 2004. As a result, its high transmittance, mobility, thermal conductivity, and outstanding mechanical and chemical stability have been proved. Especially, many researches were executed about the field of transparent electrode highlighting material of substituting the indium tin oxide (ITO). In addition, qualitative and quantitative improvements have been achieved due to many synthesis methods were discovered. Among them, mostly used method is chemical vapour deposition of graphene grown on copper or nickel. The transmittance, mobility, sheet resistance, and other many properties are completely changed according to these two types of synthesis method of graphene. In this research, considering the difference of characteristics as the synthesis method of graphene, what types of graphene should be used and how to use it were studied. The stacked graphene harvested on copper and multi-layer graphene harvested on nickel were compared and analyzed, as a result, the transmittance of 90% and the sheet resistance of $70{\Omega}{\square}$ was showed even though stacked graphene layers were 4 layers. The reason that could bring these results is lowered sheet resistance due to stacked monolayer graphenes. Moreover, light output power of the three stacked graphene spreading layer shows the highest value, but light-emitting diode with multi-layer graphene died out from 12mA due to also its high sheet resistance. Therefore, we need to clarify about what types of graphene and how to use the graphene in use.

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고온초전도 적층선재의 손실과 적층선재로 제작한 팬케이크 권선의 손실 (AC Losses of the Multi-stacked HTS tapes and Pancake Coil)

  • 이승욱;김용섭;이희준;차귀수;이지광
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2004년도 하계학술대회 논문집 B
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    • pp.776-778
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    • 2004
  • In this paper, we present effect of the stacked HTS tapes. AC losses of HTS pancake windings with stacked tapes are shown. Magnetic flux density in the HTS winding under operating conditions was calculated by FEM. AC loss of the pancake winding were measured and compared with the calculated loss by using AC losses of the stacked samples. Test results show that measured results generally agreed well with the calculated value by using AC loss of 4-stacked sample data.

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Large Area Bernal Stacked Bilayer Graphene Grown by Multi Heating Zone Low Pressure Chemical Vapor Deposition

  • Han, Jaehyun;Yeo, Jong-Souk
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2015년도 제49회 하계 정기학술대회 초록집
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    • pp.239.2-239.2
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    • 2015
  • Graphene is a most interesting material due to its unique and outstanding properties. However, semi-metallic properties of graphene along with zero bandgap energy structure limit further application to optoelectronic devices. Recently, many researchers have shown that band gap can be induced in the Bernal stacked bilayer graphene. Several methods have been used for the controlled growth of the Bernal staked bilayer graphene, but it is still challenging to control the growth process. In this paper, we synthesize the large area Bernal stacked bilayer graphene using multi heating zone low pressure chemical vapor deposition (LPCVD). The synthesized bilayer graphenes are characterized by Raman spectroscopy, optical microscope (OM), scanning electron microscopy (SEM). High resolution transmission electron microscopy (HRTEM) is used for the observation of atomic resolution image of the graphene layers.

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