• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2007년도 춘계학술대회 논문집
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• pp.285-286
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• 2007

• Journal of Magnetics
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• 제10권3호
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• pp.122-127
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• 2005

New classes of LC resonators for micro magnetic sensor device were proposed and fabricated. The first type LC resonator (Type I) consists of a small piece of microwire and two cylindrical electrodes at the end of the microwire without direct contact to its ferromagnetic core. In type I resonator the ferromagnetic core of the microwire and cylindrical electrodes act as an inductor and two capacitors respectively to form a LC circuit. The second type LC resonator (Type II) consists of a solenoidal micro-inductor with a bundle of soft magnetic microwires as a core. The solenoidal micro-inductors fabricated by MEMS technique were $500\sim1,000\;\mu{m}$ in length with $10\sim20$ turns. A capacitor is connected in parallel to the micro-inductor to form a LC circuit. A tiny glass coated $CO_{83.2}B_{3.3}Si_{5.9}Mn_{7.6}$ microwire was fabricated by a glass-coated melt spinning technique. A supergiant magneto-impedance effect was found in a type I resonator as much as 400,000% by precise tuning frequency at around 518.51 MHz. In type II resonator the changes of inductance as a function of external magnetic field in micro-inductors with properly annealed microwire cores were varied as much as 370%. The phase angle between current and voltage was also strongly dependent on the magnetic field. The drastic increments of magnetoimpedance at near the resonance frequency were observed in both types of LC resonators. Accordingly, the sudden change of the phase angle, as large as $180^{\circ}C$, evidenced the occurrence of the resonance at a given external magnetic field.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2000년도 International Symposium on Magnetics The 2000 Fall Conference
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• pp.530-531
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• 2000

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2002년도 동계연구발표회 논문개요집
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• pp.218-219
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• 2002

Recently, RF lumped-element devices are demanded strongly in application of hand-held mobile communication equipments. Many workers have been reported RF integrated inductor as well as air cores. In order to achieve the high Q value, they removed backside of substrate by micro machining process [1] and also another MEMS-like approach such as levitated structure [2]. These approaches are capable of suppressing the parasitic effects, but low reproducibility and high cost problems remain. (omitted)

• Journal of Power Electronics
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• 제17권2호
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• pp.323-333
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• 2017

This paper proposes a model-based optimal control algorithm for the clamp switch of a zero-voltage switching (ZVS) bidirectional DC-DC converter. The bidirectional DC-DC converter (BDC) can accomplish the ZVS operation using the clamp switch. The minimum current for the ZVS operation is maintained, and the inductor current is separated from the input and output voltages by the clamp switch in this topology. The clamp switch can decrease the inductor current ripple, switching loss, and conduction loss of the system. Therefore, the optimal control of the clamp switch is significant to improve the efficiency of the system. This paper proposes a model-based optimal control algorithm using phase shift in a micro-controller unit. The proposed control algorithm is demonstrated by the results of PSIM simulations and an experiment conducted in a 1-kW ZVS BDC system.

• 한국전기전자재료학회논문지
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• 제15권1호
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• pp.85-92
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• 2002

In this study, we analyzed and experimented micro-strip line inductors and capacitors for a SAW duplexer, an important devise for mobile communication. For SAW duplexers, micro-strip line lumped elements must have small impedance values, below several tens of nH or several tens of pF, and a small area pattern. In this study, we performed theoretical analysis of flat line type, meander line type, and spiral line type inductors and interdigital capacitors on a LiTaO$_3$ Piezo-crystal. We proposed a measurement method to evaluate small values of lumped elements accurately with network analyzer. In experiments, we confirmed validity of the theoretical analysis method through fabrication and characterization of micro-strip line lumped elements. The analysis method in this paper can be applied to SAW duplexers well as other microwave devices.

• Journal of Power Electronics
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• 제18권1호
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• pp.185-194
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• 2018

Interaction among multiple grid-connected inverters has a negative impact on the stable operations and power quality of a power grid. The interrelated influences of inverter inductor-capacitor-inductor filters constitute a high-order power network, and consequently, excite complex resonances at various frequencies. This study first establishes a micro-grid admittance matrix, in which inverters use deadbeat control. Multiple resonances can then be evaluated via modal analysis. For the active damping method applied to deadbeat control, the sampling frequency and the stable domain of the virtual damping ratio are also presented by analyzing system stability in the discrete domain. Simulation and experimental results confirm the efficiency of modal analysis and stable domain calculation in multi-inverter grid-connected systems.

• 한국정밀공학회지
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• 제22권9호
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• pp.7-13
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• 2005

• 한국통신학회논문지
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• 제25권5B호
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• pp.985-991
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• 2000

본 논문에서는 인덕터의 면적을 극소화시키고 인덕턴스와 Q값을 극대화시키기 위한 최적구조의 2GHz 자성박막 인덕터를 설계하고 제작하였다. Eddy-current 표피효과를 위해서 Co90Fe10와 SiO2의 multilayer를 사용하고, multilayer를 적용한 새로운 lumped 소자모델을 고려하여 최적설계를 수행하였다. 2GHz에서 동작하는 새로운 자성박막 인덕터는 photo-lithography와 lift-off기술을 이용하여 Si 기판위에 제작되었다. 50개 이상의 동일한 인덕터들의 주파수 특성은 RF Impedance Analyzer로, 자기공진주파수는 Vector Network 분석기(HP8510)로 측정되었다. 개발된 인덕터들은 1.8~2.3GHz 범위의 자기공진주파수, 47~68nH 범위의 L값, 그리고 1GHz이상의 주파수에서 70~80정도의 Q값을 가지므로 L과 Q가 극대화된 아주 우수한 최적구조의 소형(면적=30.8$\times$30.8mil2) 박막인덕터가 성공적으로 제작되었다.

• 한국자기학회지
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• 제15권1호
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• pp.30-36
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• 2005

최근 20년 동안 스핀 스프레이 방법으로 제조된 페라이트 필름이 갖는 여러 가지 우수한 점들이 보고되어 왔다. 기존의 벌크 페라이트 재료와 달리 고주파 특성이 우수하며, $100^{\circ}C$ 이하에서 저온 공정이 가능한 점이 그것이다. 따라서 상기의 방법을 이용하여 micro DC-DC 컨버터용 Ni-Zn 페라이트 인턱터를 제조하였으며, 기판재료는 폴리이미드를 사용하였고, 라미네이션과 비아홀 가공, 도금 공정을 이용하여 임베디드 형태를 완성하였다. 또한 Ni-Zn ferrite는 절연체이므로 다른 절연층을 형성하지 않았다. 제조된 Ni-Zn ferrite 는 약 0.61 T의 포화자화, 약 110의 실수 투자율을 보였고, 인덕터의 특성은 스파이럴 16턴 디자인의 경우 5 MHz에서 1.52 H에 Q-factor 24.3, 정격전류 863 mA였다.