• 대한전기학회:학술대회논문집
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• 대한전기학회 2006년도 제37회 하계학술대회 논문집 A
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• pp.593-594
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• 2006

High temperature superconducting(HTS) power cable is expected to be used for power transmission lines supplying electric power for densely populated cities in the near future. Commercializing of HTS power cable is coming. Simulation is required for safety before install of HTS power cable, a fabrication model used at the power system simulation. In this paper, we shows a single line-to ground fault analysis in the grid system which has a loom length HTS power cable. The authors developed a single line-to ground fault current calculation method which is considering the shield layer of HTS power cable. In the calculation, the T type equivalent circuit is used to derive the mutual inductance of the HTS power cable

• 대한전기학회:학술대회논문집
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• 대한전기학회 2006년도 제37회 하계학술대회 논문집 D
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• pp.2225-2226
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• 2006

High temperature superconducting(HTS) power cable is expected to be used for power transmission lines supplying electric power for densely populated cities in the near future. Commercializing of HTS power cable is coming. Simulation is required for safety before install of HTS power cable, a fabrication model used at the power system simulation. In this paper, we shows a single line-to ground fault analysis in the grid system which has a loom length HTS power cable. The authors developed a single line-to-ground fault current calculation method which is considering the shield layer of HTS power cable. In the calculation, the T type equivalent circuit is used to derive the mutual inductance of the HTS power cable.

• 대한기계학회논문집B
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• 제32권11호
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• pp.832-840
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• 2008

Ablation occurs at irradiance beyond $10^9\;W/cm^2$ with nanosecond and short laser pulses focused onto any materials. Phenomenologically, the surface temperature is instantaneously heated past its vaporization temperature. Before the surface layer is able to vaporize, underlying material will reach its vaporization temperature. Temperature and pressure of the underlying material are raised beyond their critical values, causing the surface to explode. The pressure over the irradiated surface from the recoil of vaporized material can be as high as $10^5\;MPa$. The interaction of high power nanosecond laser with a thin metal in air has been investigated. The nanosecond pulse laser beam in atmosphere generates intensive explosions of the materials. The explosive ejection of materials make the surrounding gas compressed, which form a shock wave that travels at several thousand meters per second. To understand the laser ablation mechanism including the heating and ionization of the metal after lasing, the temporal evolution of shock waves is captured on an ICCD camera through laser flash shadowgraphy. The expansion of shock wave in atmosphere was found to agree with the Sedov's self-similar spherical blast wave solution.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2008년도 제39회 하계학술대회
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• pp.808-809
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• 2008

22.9kV 50MVA HTS power cable has been developed and tested by Korea Electrotechnology Research Institute and LS Cable Company and it was supported by a grant from Center for Applied Superconductivity Technology of the 21st Century Frontier R&D Program. In this paper, DC Ic of 100m HTS cable which is installed at Kochang testing station was measured and analyzed. A measurement technique of DC Ic used by resistance and inductance removal method is established. The HTS power cable is composed of 2 layers for transmission and 1 layer for shield. For the analysis of AC losses in an HTS power cable, 2-dimensional numerical calculation was carried out to define the magnetic field distribution. We calculated the magnetization losses in the HTS core of that cable from these fields. These calculated results are in accordance with those of experiment.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2014년도 제46회 동계 정기학술대회 초록집
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• pp.232.2-232.2
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• 2014

Since its discovery in 2004, graphene, a sp2-hybridized 2-Dimension carbon material, has drawn enormous attention. A variety of approaches have been attempted, such as epitaxial growth from silicon carbide, chemical reduction of graphene oxide and CVD. Among these approaches, the CVD process takes great attention due to its guarantee of high quality and large scale with high yield on various transition metals. After synthesis of graphene on metal substrate, the subsequent transfer process is needed to transfer graphene onto various target substrates, such as bubbling transfer, renewable epoxy transfer and wet etching transfer. However, those transfer processes are hard to control and inevitably induce defects to graphene film. Especially for wet etching transfer, the metal substrate is totally etched away, which is horrendous resources wasting, time consuming, and unsuitable for industry production. Thus, our group develops one-step process to directly grow graphene on glass substrate in plasma enhanced chemical vapor deposition (PECVD). Copper foil is used as catalyst to enhance the growth of graphene, as well as a temperature shield to provide relatively low temperature to glass substrate. The effect of growth time is reported that longer growth time will provide lower sheet resistance and higher VSG flakes. The VSG with conductivity of $800{\Omega}/sq$ and thickness of 270 nm grown on glass substrate can be obtained under 12 min growing time. The morphology is clearly showed by SEM image and Raman spectra that VSG film is composed of base layer of amorphous carbon and vertically arranged graphene flakes.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2006년도 제37회 하계학술대회 논문집 B
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• pp.1259-1260
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• 2006

High temperature superconducting(HTS) power cable is expected to be used for power transmission lines supplying electric power for densely populated cities in the near future. Commercializing of HTS power cable is coming. Simulation is required for safety before install of HTS power cable, a fabrication model used at the power system simulation. In this paper, we shows a single line-to ground fault analysis in the grid system which has a 100m length HTS power cable. The authors developed a single line-to-ground fault current calculation method which is considering the shield layer of HTS power cable. In the calculation, the T type equivalent circuit is used to derive the mutual inductance of the HTS power cable.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2006년도 제37회 하계학술대회 논문집 C
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• pp.1719-1720
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• 2006

High temperature superconducting(HTS) power cable is expected to be used for power transmission lines supplying electric power for densely populated cities in the near future. Commercializing of HTS power cable is coming. Simulation is required for safety before install of HTS power cable, 3 fabrication model used at the power system simulation. In this paper, we shows a single line-to ground fault analysis in the grid system which has a loom length HTS power cable. The authors developed a single line-to-ground fault current calculation method which is considering the shield layer of HTS power cable. In the calculation, the T type equivalent circuit is used to derive the mutual inductance of the HTS power cable.

• 한국재료학회지
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• 제15권11호
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• pp.745-750
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• 2005

Polycarbonates are widely used as housing materials of electronic handsets. Since the polycarbonate is electrically insulating, there should be a conducting layer on the polycarbonate for EMI shielding. In this study, we sputter deposited Cu films on the polycarbonate substrates for EMI shielding. Plasma treatments of polycarbonates were used to increase the adhesion strength of the Cu film/polycarbonate interface. The surface energy of the polycarbonate was greatly increased from $30mJ/m^2 \;to\; 65mJ/m^2$ by a 200 W $O_2$ plasma treatment for 10s. It is thought that this is because of the ion bombardment. The adhesion strength of the sputter deposited Cu film to the polycarbonate was quantitatively measured by a 4 point bending tester. A moderate plasma surface treatment of the polycarbonate increased the Cu film/polycarbonate adhesion strength by $30\%$. The EMI shielding efficiency of the sputter deposited $10{\mu}m$ Cu lam on the polycarbonate showed 90dB in the range of 100MHz to 1000MHz.

• 한국지형학회지
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• 제19권4호
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• pp.39-57
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• 2012

울릉도 화산체는 해수면 아래의 순상화산체와 해수면 위의 종상화산체로 크게 구분된다. 해수면 위 화산체의 지질은 기본적으로 알칼리 화산암류이며 이들은 다시 집괴암 및 응회암, 조면암 및 포놀라이트, 조면암질 부석, 조면안산암, 퇴적층 등 5개 지층으로 구분된다. 울릉도 지형은 전체적으로 화산지형이 우세하며 이들 화산지형이 풍화, 침식되어 다양한 풍화지형, 하천지형, 해안지형, 구조지형 등이 만들어졌다. 주요 화산지형으로는 칼데라분지, 중앙화구구, 주상절리 등이 있으며, 풍화지형으로는 타포니, 나마, 토르, 풍화동굴, 애추 등이 있다. 주요 해안지형으로는 해식애, 파식대, 시스택, 시아치, 해식동, 자갈해빈, 해안단구 등이 있다. 하천지형은 폭포를 제외하고는 그 발달이 미약하다.

• 한국콘텐츠학회논문지
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• 제8권11호
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• pp.182-188
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• 2008

최근 방사선치료의 중추적 역할을 담당하고 있는 다엽콜리메이터는 사용의 편리성 때문에 기존의 납합 금 차폐물을 급속도로 대체하고 있다. 그러나 다엽콜리메이터는 엽간 누설선량이나 디지털 신호를 입출력 알고리즘에 따른 오류가 발생할 수 있다. 저자는 미국 Varian사에서 제공하는 다엽콜리메이터의 입력 방법에 따른 차이를 모의치료장치 프로그램(XimaVision)값을 기준으로 전자펜 정보 전송장치(MLC shaper)와 디지털 변환장치(film scanner)에서의 오차와 유효 조사야를 여러 형태의 차폐윤곽으로 비교하였다. 기준 값과 비교하여 기본적인 차폐 윤곽(test1-5)에서 전자펜 전송방식은 $0{\sim}0.29cm$, $0.23{\sim}3.59cm^2$, 디지털 변환장치 방식은 $0{\sim}0.20cm$, $0.72{\sim2.59cm^2$ 차이를 보였다. 임상에서 적용되는 차폐 윤곽에서 전자펜 전송방식은 $0{\sim}0.54cm$, $0.04{\sim}1.68cm^2$, 디지털 변환장치 방식은 $0{\sim}0.78cm$, $0.24{\sim}3.89cm^2$ 차이를 보였고, 대부분 선속 중심선에서 멀어질수록 조사야가 클수록 오차범위가 증가함을 알 수 있었다. 다엽콜리메이터의 임상적용을 위한 다양한 정보 입력과정에서 기준점으로부터 수 mm 이내에서 오차가 잇었다. 그리고 유효 조사야는 실제 면적에 대하여 수 $cm^2$이내에서 오차가 발생하여 기계적 선량(Monitor Unit)이나 조사야 내 선량변화에 관여하지 않았다. 그러나 임계장기를 차폐 할 경우 장기의 움직임으로 표적용적의 일부가 포함되지 않을 수 있기 때문에 문제의 여지가 있다. 그러므로 오류를 최소화하기 위한 다엽콜리메이터의 입력과정에 세심한 주의를 기울여야 한다.