• 한국진공학회:학술대회논문집
• /
• 한국진공학회 2016년도 제50회 동계 정기학술대회 초록집
• /
• pp.247.1-247.1
• /
• 2016

Low-cost, high efficiency solar cells are tremendous interests for the realization of a renewable and clean energy source. ZnTe based solar cells have a possibility of high efficiency with formation of an intermediated energy band structure by impurity doping. In this work, ZnO/ZnTe:Cr and ZnO/i-ZnTe structures were fabricated by pulsed laser deposition (PLD) technique. A pulsed (10 Hz) Nd:YAG laser operating at a wavelength of 266 nm was used to produce a plasma plume from an ablated a ZnTe target, whose density of laser energy was 10 J/cm2. The base pressure of the chamber was kept at approximately $4{\times}10-7Torr$. ZnTe:Cr and i-ZnTe thin films with thickness of 210 nm were grown on p-Si substrate, respectively, and then ZnO thin films with thickness of 150 nm were grown on ZnTe:Cr layer under oxygen partial pressure of 3 mTorr. Growth temperature of all the films was set to $250^{\circ}C$. For fabricating ZnO/i-ZnTe and ZnO/ZnTe:Cr solar cells, indium metal and Ti/Au grid patterns were deposited on back and front side of the solar cells by using thermal evaporator, respectively. From the fabricated ZnO/ZnTe:Cr and ZnO/i-ZnTe solar cell, dark currents were measured by using Keithley 2600. Solar cell parameters were obtained under Air Mass 1.5 Global solar simulator with an irradiation intensity of 100 mW/cm2, and then the photoelectric conversion efficiency values of ZnO/ZnTe:Cr and ZnO/i-ZnTe solar cells were measured at 1.5 % and 0.3 %, respectively.

• 대한기계학회논문집B
• /
• 제30권6호
• /
• pp.553-559
• /
• 2006

Most diesel injector, which is currently used in high-pressure common rail fuel injection system of diesel engine, is driven by the solenoid coil energy for its needle movement. The main disadvantage of this solenoid-driven injector is a high power consumption, high power loss through solenoid coil and relatively fixed needle response's problem. In this study, a prototype piezo-driven injector, as a new injector mechanism driven by piezoelectric energy based on the concept of inverse piezo-electric effect, has been designed and fabricated to know the effect of piezo-driven injection processes on the diesel spray structure and internal nozzle flow. Firstly we investigated the spray characteristics in a constant volume chamber pressurized by nitrogen gas using the back diffusion light illumination method for high-speed temporal photography and also analyzed the inside nozzle flow by a fully transient simulation with cavitation model using VOF(volume of fraction) method. The numerical calculation has been performed to simulate the cavitating flow of 3-dimensional real size single hole nozzle along the injection duration. Results were compared between a conventional solenoid-driven injector and piezo-driven injector, both equipped with the same micro-sac multi-hole injection nozzle. The experimental results show that the piezo-driven injector has short injection delay and a faster spray development and produces higher injection velocity than the solenoid-driven injector. And the predicted simulation results with the degree of cavitation's generation inside nozzle for faster needle response In a piezo-driven injector were reflected to spray development in agreement with the experimental spray images.

• 동력기계공학회지
• /
• 제16권4호
• /
• pp.30-36
• /
• 2012

A scroll expander has been designed to produce a shaft power from a R134a Rankine cycle for electricity generation. Heat was supplied to the Rankine cycle through a heat exchanger, which received heat from another cycle of water. In the water cycle, water was heated up in a boiler using biogenic solid fuel. The designed scroll expander was a horizontal type, and a trochoidal oil pump was employed for oil supply to bearings and Oldham-ring keys. For axial compliance, a back pressure chamber was created on the backside of the orbiting scroll base plate. Numerical study has been carried out to estimate the performance of the designed scroll expander. The expander was estimated to produce the shaft power of about 2.9 kW from a heat supply of 36 kW, when the temperature of R134a was $80^{\circ}C$ and $35^{\circ}C$ at the evaporator and condenser of the Rankine cycle, respectively. The expander efficiency was about 70.5%. When the amount of heat supply varied in the ranges of 7.5~55 kW, the expander efficiency changed in the range of 45.6~70.5%, showing a peak efficiency of 70.5% at the design shaft speed.

• Journal of Radiation Protection and Research
• /
• 제35권2호
• /
• pp.57-62
• /
• 2010

원전 계획예방정비기간 증기발생기 수실작업, 가압기 전열관교체 또는 압력관피더 제거작업 지역 등은 높은 방사선량률을 보이는 지역으로, 짧은 시간 동안의 작업으로 작업종사자는 높은 피폭을 받을 가능성이 있다. 특히, 방사성물질과 접촉하는 손 부위는 높은 피폭이 일어날 수 있다. 이런 점을 고려하여 국내 가압경수로원전과 가압중수로원전의 계획 예방정비기간 중 증기발생기 수실 노즐댐 설치와 제거작업, 원자로 냉각재펌프 보수작업, 원자로헤드 보수 및 검사작업 등과 같은 고피폭 접촉작업에서 방사선작업종사자의 말단선량을 측정하기위한 현장시험을 실시하였다. 여기에 참여한 작업종사자는 가슴과 등 부위에 일상적인 절차에 따른 복수선량계를 패용한 것 이외에 손목에 개인선량계를 추가로 패용하였고, 손가락 부위에는 말단선량계 (Extremity dosimeter)를 패용하였다. 그 결과, 손가락이 받는 등가선량은 각각 손목이 받는 등가선량 및 가슴 또는 등 부위가 받는 등가선량과 일정한 비율로 평가됨을 확인하였다.

• 한국수산과학회지
• /
• 제10권4호
• /
• pp.227-235
• /
• 1977

1976년 8월 16일 (북위 $34^{\circ}27'30'$ 동경 $128^{\circ}23'15'$)과 1977넌 7월 28일(북위 $34^{\circ}47'$ 동경 $128^{\circ}53'$)에 관악산호의 선박소음이 r.p.m에 따라 항해시와 정선시 (기관의 공회전)의 소음압이 해중에 분포하는 것을 조사 연구한 결과를 요약하면 다음과 같다. 1. 기관의 r.p.m.과 음압관계 r.p.m.과 음압의 증가비는 100 : 1이었으며 r.p.m. 600에서 104dB로 peak를 이루었다. 2. 외현주변의 해중해압분포 A. 정선시의 기관소음압 100,102,103,104,104 dB일때 관측점 No.1에서 69,70,72,74,75 dB No.3은 No. 1에 비해 $2\~3\;dB$ 증가해 peak를 이루었고 No.5는 No.3에 비해 $10\~15\;dB$씩 감쇠되었다. 기관소음압이 최대 일때 관측점 $No.1\~No.5$에서의 음압이 투과된 백분율은 약 $78,79,80,73,70\%$였다. B. 항해시의 선박수중소음압 정선시와 같은 기관회전 조건하에서 No.2에서 69,72,75,77,78 dB로 peak를 이고 No. 1보다 $2\~3\;dB$씩 감쇠되었다. 기관 최고소음압에 대한 $No1.\~No.5$에서의 음압투과 백분율은 약 $78,81,79,77,71\%$ 였다. 3. 항해시와 정선시의 외현해중 음압 peak점에서의 음압을 비교하면 항해시가 1 dB 높았다. 4. 선박이 멀어질 때 0 m(관측점 통과시)에서 67 dB, 1,400 m에서 56 dB였다. 5. 선박이 가까워질 때 거리 0 m에서 72 dB, 1,400 m에서 57 dB로서 멀어 질때와 비교하면 0m에서 5 dB, 600 m에서 2 pB씩 증가한 도플러 효과가 일어남을 알 수 있다. 6. r.p.m.을 600으로 하여놓고 스크류를 돌리지 않고 기관만 공회전 시킬 때 수평거리 20 m인 곳의 No.7에서 수심 10 m마다 50 m까지의 음압은 68,75,62,59,55,51 dB였다.

• 한국진공학회:학술대회논문집
• /
• 한국진공학회 2013년도 제45회 하계 정기학술대회 초록집
• /
• pp.221-221
• /
• 2013

Vertical LED (VLED) has been recognized as a way to obtain the high-power LED due to their advantages [1]. However, approximately 4% of the light generated from the active region is extracted, if the light extraction from side walls and back side is neglected because of Fresnel reflection (FR) and total internal reflection (TIR) [2,3]. In this study, the optical simulation of the VLED with the various microstructures was performed. Among them, the microlens having the diameter of 3 ${\mu}m$ and the height of 1.5 ${\mu}m$ shown the best result was chosen, and then, optimized microlens was formed on a GaN template using conventional semiconductor process. Various microstructures were proposed to improve the light extraction efficiency (LEE) of the VLED for the simulation. The LEE was simulated using LightTools based on a Monte Carlo ray tracing. The microstructures with hemisphere, cone, truncated and cylinder pattern having diameter of 3 ${\mu}m$ were employed on the top layer of the VLED respectively. The improvement of the LEE by using the microstructure is 87% for the hemisphere, 77% for the cone, 53% for the truncated, 21% for the cylinder, compared with the LEE of the flat surface at the reflectance of 85%. The LEE was increased by 88% at the height of 1.5 ${\mu}m$, compared with the LEE of the flat surface. We found that the microlens on the top layer is the most suitable for increasing the LEE. In order to apply the proposed microlens on n-GaN surface, we fabricated microlens on a GaN template. A photoresist array having hexagonal-closed packed microlens was fabricated on the GaN template. Then, optimization of etching the GaN template was performed using a dry etching process with ICP-RIE. The dry etching carried out using a gas mixture of Cl2 and Ar, each having a flow rate of 16 sccm and 10 sccm, respectively with RF power of 50 W, ICP power of 900 W and chamber pressure of 2 mTorr was the optimum etching condition as shown in Fig. 2(a).