• 한국자기학회지
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• 제24권3호
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• pp.76-80
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• 2014

토로이드 형태의 자성분말합금 코어의 경우 major B-H loop을 측정하기 위해서는 수십 kA/m 이상의 높은 자화력을 인가하여야 한다. 이 경우 측정과정에서 일차코일에 권선된 에나멜 동선에서 발생하는 열 때문에 측정이 매우 어렵다. 본 연구에서는 토로이드 형태의 자성분말합금 코어 major B-H loop을 직접 측정할 수 있는 장치를 설계 제작하고, 그 성능을 측정하였다. 수십 kA/m 이상의 자화력을 인가하기 위하여 최대 전류가 $100A_P$인 전력 증폭기와 측정 시간 중에 높은 전류에 의하여 코일 권선에서 발생하는 열 문제를 해결하기 위하여 실시간으로 자기 이력 곡선을 측정 할 수 있게 실시간으로 B-H 신호를 디지털신호로 변환하여 컴퓨터 소프트웨어에서 자속밀도 B 와 자화력 H 값을 계산하고, 이 값들로 부터 주요 자기 특성인 최대자속밀도 $B_{max}$, 최대 자화력 $H_{max}$, 보자력 $H_c$, 잔류자속밀도 $B_r$ 및 형상인자(FF)를 계산하여 가상계측기(VI)창으로 표시 할 수 있게 하였다. 제작된 장치를 이용하여 외경이 134 mm, 내경이 77 mm, 높이가 42 mm인 자성분말코어에 일차 코일을 직경이 1 mm인 에나멜 동선을 401회 권선하고 이차 코일을 직경이 0.2 mm인 에나멜 동선 5회 권선하여 측정을 하여 본 결과 최대 인가 자기장을 50 kA/m까지 인가하면서 자기이력곡선을 측정 할 수 있었다.

• 한국정밀공학회지
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• 제22권7호
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• pp.94-101
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• 2005

This work proposes a new method for describing the hysteresis non-linearity of a piezoelectric actuator. The hysteresis behaviour of piezoelectric actuators, including the minor loop trajectory, are modeled by geometrical relationship between a reference major loop and its minor loops. This hysteresis model is transformed into inverse hysteresis model in order to output compensated voltage with regard to the given input displacement. A feedforward neural network, which is trained by a feedback PID control module, is incorporated to the inverse hysteresis model to compensate unknown dynamics of the piezoelectric system. To show the feasibility of the proposed feedforward-feedback controller, some experiments have been carried out and the tracking performance was compared to that of simple PTD controller.

• 제어로봇시스템학회논문지
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• 제8권9호
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• pp.736-746
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• 2002

There has been a great demand for smart actuators in the field of micro-machines. However, the control accuracy of smart actuators, e.g., a shape memory alloy(SMA) and a piezoceramic actuator, is limited due to the inherent hysteresis nonlinearity. The Preisach hysteresis model has emerged as an appropriate model f3r the behavior of those smart actuators. Yet it is still not easy to construct a practical model of hysteresis using the classical Preisach model. Accordingly, in this paper, we propose a new simple method for modeling of the hysteresis nonlinearity of SMA. Using only the proportional relation of the major loop of hysteresis, the proposed method makes the computation of the Preisach model easy. We prove the efficacy of the proposed model through the comparative the experimentation with the classical Preisach model.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2005년도 춘계학술대회 논문집
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• pp.1074-1078
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• 2005

In precision positioning applications, such as scanning tunneling microscopy and diamond turning machines [1], it is often required that actuators have nanometer resolution in displacement, high stiffness, and fast frequency response. These requirements are met by the use of piezoceramic actuators. A major limitation of piezoceramic actuators, however, is their lack of accuracy due to hysteresis nonlinearity and drift. The maximum error due to hysteresis can be as much as 10-15% of the path covered if the actuators are run in an open-loop fashion. Hence, the accurate control of piezoceramic actuators requires a control strategy that incorporates some form of compensation for the hysteresis. One approach is to develop an accurate model of the hysteresis and the use the inverse as a compensator. The Preisach model has frequently been employed as a nonlinear model for representing the hysteresis, because it encompasses the basic features of the hysteresis phenomena in a conceptually simple and mathematically elegant way. In this paper, a new numerical inversion scheme of the Preisach model is developed with an aim of compensating hysteresis in piezoceramic actuators. The inversion scheme is implemented using the first-order reversal functions and is presented in a recursive form. The inverted model is then incorporated in an open-loop control strategy that regulates the piezoceramic actuator and compensates for hysteretic effects. Experimental results demonstrate satisfactory regulation of the position of the piezoceramic actuator to the desired trajectories.

• Journal of Magnetics
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• 제6권2호
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• pp.66-69
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• 2001

The actual magnetic induction waveform of cores in electrical machines is not sinusoidal i.e. higher harmonics are always included. Thus the core loss in actual electrical machines is different from the core loss which is measured by the standard method, because the waveform of magnetic induction should be sinusoidal in the standard testing method. Core loss analysis under higher harmonic induction is always important in electric machine design. In this works we measured the core loss when a hysteresis loop has only one period of an ac minor loop of higher harmonic frequency, depending on the position of the ac minor loop of relative to the fundamental harmonic frequency. From this experiment, the core loss P(B/sub 0/f/sub 0/, B/sub h/, nf/sub 0/)) under a higher harmonic magnetic induction B/sub h/ could be expressed by the linear combination the core loss at fundamental harmonic frequency P/sub c/(B/sub 0/, f/sub 0/), the core loss of ac minor loop at zero induction region of the major hysteresis loop P/sub cL/ (B/sub h/, nf/sub 0/), and the core loss of an ac minor loop in the high induction region of the major hysteresis loop P/sub cH/ (B/sub h/, nf/sub 0/) i.e., P/sub c/, (B/sub 0/, f/sub 0/, B/sub h/, nf/sub 0/)=P/sub c/ (B/sub 0/, f/sub 0/,)+(n-1)[k₁(B/sub 0/) P/sub cL/ (B/sub h/, nf/sub 0/)+(1-k₁(B/sub 0/)) P/sub cH/ (B/sub h/, nf/sub 0/)]. This will be useful formula for electrical machine designers and one of effective methods to predict core loss including higher harmonic induction.

• KIEE International Transaction on Electrical Machinery and Energy Conversion Systems
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• 제2B권4호
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• pp.168-173
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• 2002

A new identification algorithm for the Preisach model is presented. The algorithm treats the identification procedure of the Preisach model as an inverse problem where the independent variables are parameters of the distribution function and the objective function is constructed using only the initial magnetization curve or only tile major loop of the hysteresis curve as well as the whole reversal curves. To parameterize the distribution function, the Bezier spline and Gaussian function are used for the coercive and interaction fields axes, respectively. The presented algorithm is applied to the ferrite permanent magnets, and the distribution functions are correctly found from the major loop of the hysteresis curve or the initial magnetization curve.

• 한국광학회:학술대회논문집
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• 한국광학회 1988년도 광학 및 양자전자학 워크샵
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• pp.127-131
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• 1988

In order to clarify the origin of perpendicular anisotropy in thermally evaporated TbFeCo amorphous thin films, we have investigated the effects of deposition angle on magnetic Kerr hysteresis loop, perpendicular magnetic anisotropy and internal stress depend strongly on the deposition angle and above a threshold value(30$^{\circ}$), the perpendicular anisotropy disapperars and the in-plane anisotropy appears. The measurement of internal stress is the major contribution to the perpendicular anisotropy. The measurements of Kerr hysteresis loops in the polar and the longitudinal directions show that as the deposition angle increases the polar kerr hystresis loop deteriorates while the longitudinal Kerr hystersis loop becomes prominent.

• 한국해안·해양공학회논문집
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• 제22권5호
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• pp.316-325
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• 2010

황해중부해역에 설치된 황해 모니터링 부이에서 관측한 기온과 표층수온의 변동성분을 추출하기 위하여 조화분석을 수행하였다. 분석결과, 기온과 표층 수온 모두 1년, 반년 주기성분이 가장 우세한 것으로 파악되었으며, 보다 짧은 주기성분은 $0.2{\sim}0.5^{\circ}C$ 이하의 작은 변동성분에만 기여하는 것으로 파악되었다. 한편, 기온과 표층수온의 조화분석 성분에서 추출한 잔차성분을 분석한 결과, 기온 잔차성분의 표준편차는 표층 수온 잔차성분의 표준편차보다 2.4배 정도 크고, 잔차성분의 발생빈도분포는 정규분포로 근사화하는 것이 가능한 것으로 파악되었다. 한편, 기온에 따른 표층수온 변화양상을 기온-표층수온 평면에서 분석한 결과 뚜렷한 연속적인 이력고리(hysteresis loop)를 형성하는 것이 발견되었으며, 반시계방향의 기온-표층수온 상승기, 기온-표층수온 하강기 그리고 동계 일정한 표층수온 유지기로 구성되어 있는 것으로 파악되었다.

• 한국전산구조공학회:학술대회논문집
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• 한국전산구조공학회 2008년도 정기 학술대회
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• pp.331-336
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• 2008

An self-centering energy-dissipative (SCED) bracing system has recently been developed as a new seismic force resistant bracing system. The advantage of the SCED brace system is that, unlike other comparable advanced bracing systems that dissipate energy, such as the buckling restrained brace system, it has a self-centering capability that reduces or eliminates residual building deformations after major seismic events. In this study seismic performance of SCED braced frames is evaluated for a set of 20 design level earthquake records. According to analysis results the SCED systems showed more uniform interstory drift demand for buildings with 8 story or fewer. The residual deformation in SCED buildings turned out to be much less than that of moment-resisting frames.

• 대한전기학회:학술대회논문집
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• 대한전기학회 1996년도 하계학술대회 논문집 A
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• pp.56-58
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• 1996

The Preisach model needs a density function to simulate the hysteresis phenomena. To obtain this function, many experimental data obtained from the first order transition curves are required to get accurate density function. However, it is difficult to perform this procedure, especially for the hard magnetic materials. In this paper, we compare the density function obtained from the experimental data with that computed from the mathematical function like the Gaussian function, and propose a simple technique to get mathematical equation of the density function or Everett function which is obtained from the initial curve, major and minor loop.