• 한국표면공학회지
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• 제29권5호
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• pp.474-477
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• 1996

The solid state cesium ion beam sputter deposition system has been developed for negative carbon ion beam deposition. The negative carbon ion beams are effectively produced by cesium ion bombardment. The C-ion beam current and deposition energy can be independently controlled for the deposition of a-D films. This system is very compact, reliable and high flux without any gas discharge or plasma and has been successfully used in the studies of the ion beam deposited amorphous diamond(a-D)

• 한국항공우주학회지
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• 제35권2호
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• pp.115-123
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• 2007

본 논문은 리튬이온 (Li-ion) 셀을 채용한 인공위성용 전력계의 개념 설계에 대하여 기술한다. 기존의 니켈카드뮴 (NiCd) 셀과 비교할 때, 리튬이온 (Li-ion) 셀은 에너지 밀도, 무게 그리고 부피에서 큰 잇점을 갖고 있다. 니켈카드뮴 (NiCd) 셀의 평균 출력전압은 +1.2V이며, 리튬이온 (Li-ion) 셀의 출력전압은 +3.6V이다. 그러나, 리튬이온 (Li-ion) 셀의 충전과 방전에 있어서의 절차는 기존의 니켈카드뮴 (NiCd) 셀 보다는 어렵다. 따라서, 리튬이온 (Li-ion) 셀의 충전과 방전 시에는 각각의 셀에 대하여 충전 전압과 방전 전압을 검침하고 제어를 해주어야 하므로 별도의 제어 회로가 요구된다. 따라서, 본 논문을 통하여 리튬이온 (Li-ion) 셀을 채용한 전력계의 설계 시 고려하여야 할 사항 및 리튬이온 (Li-ion) 셀의 충방전 특성에 대한 연구 결과를 제시하고자 한다.

• 방사성폐기물학회지
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• 제3권4호
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• pp.269-278
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• 2005

본 논문에서는 불필요한 용액의 발생이 없이 전해 반응계로 주입되는 용액을 오직 pH 만 조절시켜 배출시키기 위한 연속식 이온교환막 전해 시스템을 개발하였다. 여기서는 전해 반응기 앞에 한 pH-조정조를 두고 대상 용액을 pH-조정조로 주입하면서 pH-조정조의 용액의 일부를 이온 교환막에 따라 음극방 또는 양극방으로 거처 다시 pH-조정조로 순환하게 하며, pH-조정조의 용액의 일부를 상대극 방으로 통과시킴으로써 pH가 조절되어 배출되게 하였다. 양이온 교환막을 사용하는 경우 음극방을 거치는 용액을 pH-조정조로 순환하게 하고, 음이온 교환막을 사용하는 경우 양극방을 거치는 용액을 pH-조정조로 순환하게 함으로서 배출되는 용액을 효과적으로 산성용액 또는 알카리용액으로 만들 수 있었다. 이러한 전해반응기에서 pH 조절 과정은 음극과 양극 사이에 전압 차가 형성될 시, 이온교환막을 통한 용액 중 이온의 전기이동 현상에 의해 유발되는 음극방과 양극방에서 용액의 전하 비 평형 현상과 이에 따른 물의 전해 분해과정에 의해 설명되었다.

• 전력전자학회:학술대회논문집
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• 전력전자학회 2008년도 하계학술대회 논문집
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• pp.259-261
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• 2008

The electronic products such as laptop PC, cellular phone, robots and etc. need the DC power source. Recently, the secondary battery is frequently used as the portable DC power source and it needs forming process. In this paper, we proposed the bidirectional converter that the battery can be charged with high power factor and the discharged energy is regenerated into AC power source. In the charging mode, the converter acts as the boost rectifier. And the AC input current is controlled in phase with the AC input voltage. As a result, the power factor is improved nearly to unity. In the discharging mode, the DC power of battery wasted in resistor is regenerated to the AC bus line. Finally, the validity of the proposed bidirectional converter is verified by computer simulations and experimentation.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2000년도 하계학술대회 논문집 C
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• pp.2107-2109
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• 2000

A pulsed Nd:YAG laser is used widely for materials processing and medical instrument. It's very important to control the laser energy density in those fields using a pulsed Nd:YAG laser. A pulse repetition rate and a pulse width are regarded as the most dominant factors to control the energy density of laser beam. In this paper, the alternating charge and discharge system was designed to adjust a pulse repetition rate This system is controlled by microprocessor and allows to replace an expensive condenser for high frequency to cheap one for low frequency. In addition, The microcontroller monitors the flow of cooling water, short circuit. and miss firing and so on. We designed Nd:YAG laser firmware with smart microcontroller, and want to explain general matters about the firmware from now.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2005년도 제36회 하계학술대회 논문집 C
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• pp.2138-2139
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• 2005

We demonstrate a simple CO2 laser by controlling firing angle of a TRIAC switch in ac power line. The power supply for our laser system switches the voltage of the AC power line (60Hz) directly. The power supply does not need elements such as a rectifier bridge, energy-storage capacitors, or a current-limiting resistor in the discharge circuit. In order to control the laser output power, the pulse repetition rate is adjusted up to 60Hz and the firing angle of TRIAC gate is varied from 45 to 135. A ZCS(Zero Crossing Switch) circuit and a PIC one-chip microprocessor are used to control the gate signal of the TRIAC precisely. The maximum laser output of 40W is obtained at a total pressure of 18Torr, a pulse repetition rate of 60Hz, and a TRAIC gate firing angle of 90.

• 한국수소및신에너지학회논문집
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• 제32권4호
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• pp.197-204
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• 2021

Pressure swing adsorption is a purification process which can get pure hydrogen. The purification process is composed of four process: compression, adsorption, desorption and discharge. In this study the adsorption process was simulated by using the Fluent and validated with experimental results. A gas used in experiment is composed of H₂, CO₂, CH₄, and CO. Adsorption process conducted under 313 kelvin and 3 bar and bituminous-coal-based (BPL) activated carbon was used as the adsorbent. Langmuir model was applied to explain the gas adsorption. And diffusion of all the gases was controlled by micro-pore resistances. The result shows that, the most adsorbed gas was carbon dioxide, followed by methane and carbon monoxide. And carbon monoxide took the least amount of time to reach the maximum adsorption amount. The molar fraction of the off-gas became the same as the molar fraction of the gas supplied from the inlet after adsorption reached the equilibrium.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2012년도 제43회 하계 정기 학술대회 초록집
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• pp.269-269
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• 2012

A new ion source has been designed, fabricated, and installed at the NBTS (Neutral Beam Test Stand) at the KAERI (Korea Atomic Energy Research Institute) site. The goalis to provide a 100 keV, 2MW deuterium neutral beam injection as an auxiliary heating of KSTAR (Korea Super Tokamak Advanced Research). To cope with power demand, an ion current of 50 A is required considering the beam power loss and neutralization efficiency. The new ion source consists of a magnetic cusp bucket plasma generator and a set of tetrode accelerators with circular copper apertures. The plasma generator for the new ion source has the same design concept as the modified JAEA multi-cusp plasma generator for the KSTAR prototype ion source. The dimensions of the plasma generator are a cross section of $59{\times}25cm^2$ with a 32.5 cm depth. The anode has azimuthal arrays of Nd-Fe permanent magnets (3.4 kG at surface) in the bucket and an electron dump, which makes 9 cusp lines including the electron dump. The discharge properties were investigated preliminarily to enhance the efficiency of the beam extraction. The discharge of the new ion source was mainly controlled by a constant power mode of operation. The discharge of the plasma generator was initiated by the support of primary electrons emitted from the cathode, consisting of 12 tungsten filaments with a hair-pin type (diameter = 2.0 mm). The arc discharge of the new ion source was achieved easily up to an arc power of 80 kW (80 V/1000 A) with hydrogen gas. The 80 kW capacity seems sufficient for the arc power supply to attain the goal of arc efficiency (beam extracted current/discharge input power = 0.8 A/kW). The accelerator of the new ion source consists of four grids: plasma grid (G1), gradient grid (G2), suppressor grid (G3), and ground grid (G4). Each grid has 280 EA circular apertures. The performance tests of the new ion source accelerator were also finished including accelerator conditioning. A hydrogen ion beam was successfully extracted up to 100 keV /60 A. The optimum perveance is defined where the beam divergence is at a minimum was also investigated experimentally. The optimum hydrogen beam perveance is over $2.3{\mu}P$ at 60 keV, and the beam divergence angle is below $1.0^{\circ}$. Thus, the new ion source is expected to be capable of extracting more than a 5 MW deuterium ion beam power at 100 keV. This ion source can deliver ~2 MW of neutral beam power to KSTAR tokamak plasma for the 2012 campaign.

• 전기화학회지
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• 제18권1호
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• pp.31-37
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• 2015

삼성분 칼코게나이드 화합물인 황화 주석 저마늄 ($Sn_xGe_{1-x}S$) 합금 나노입자를 메틸 주석 $(Sn(CH_3)_4$, tetramethyl tin, TMT) 메틸 저마늄 $(Ge(CH_3)_4$, tetramethyl germanium, TMG), 황화수소 ($H_2S$, hydrogen sulfide) 혼합 가스의 레이저 광분해 반응법으로 합성할 수 있으며, 이때 반응기 안의 가스 혼합비율에 따라 나노입자의 주석과 저마늄의 조성비를 조절할 수 있었다. 조성비를 가변시킨 나노입자는 모두 결정성을 갖게 만들 수 있었으며, 리튬 이온 전지의 음극소재로서 우수한 특성을 보여주었다. 조성비에 따라 특성을 조사결과, 황화저마늄은 70 사이클 후 최대 1200 mAh/g의 가장 높은 방전용량을 갖는 것과, 주석 성분 함량이 클수록 높은 충방전률에서 용량 유지가 더 잘 됨을 확인하였다. 이와 같은 우수한 효율의 황화물 합금 나노입자의 새로운 대량 합성법은 고성능 에너지 변환 소재 실용화에 기여할 것으로 예상된다.

• 전기학회논문지
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• 제63권5호
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• pp.622-628
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• 2014

This paper presents the SOC-based control strategy of BESS(Battery Energy Storage System) for providing power system frequency regulation in the bulk power systems. As the life cycle of BESS would be shortened by frequent changes of charge and discharge required for frequency regulation in a steady state, the proposed algorithm operates BESS within a range of SOC where its life cycle can be maximized. However, during a transient period of which occurrence frequency is low, BESS would be controlled to use its full capacity in a wider range of SOC. In addition, each output of multiple BESS is proportionally determined by its SOC so that the balance in SOC of multiple BESS can be managed. The effectiveness of the proposed control strategy is verified through various case studies employing a test system. Moreover, the control result of BESS with the measured frequency from a real system shows SOC of BESS can be maintained within a specific range although the frequency deviation is biased.