• 한국자기학회지
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• 제6권1호
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• pp.1-6
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• 1996

MR/TbCo 박막 계면의 자기교환 결합의 특성을 시뮬레이션 하기 위해서 박막내에 존재 하는 자기 에너지를 최소화 하여 자화의 방향을 구하였다. 수치해석 방법으로는 Newton법과 Gauss-Seidel 방법이 이용되었다. TbCo의 이방성 상수에 비례적으로 자기 이력곡선의 폭이 변하고, TbCo 천이영역의 두께가 얇을수록 자기이력곡선이 벌어지지 않았다. 특히 TbCo 천이영역의 두께가 $400\;\AA$ 일때 단일 곡선(보자력 10 Oe 이하)을 보였다. 또한 계면 교환 결합상수가 작을수록 천이영역의 두께가 얇을 때와 비슷한 곡선을 보였고, 완전히 결합된 상태의 1/100 정도 일때, 단일 곡선을 보였다. 제작한 박막의 자기이력곡선과 비교하여 계면교환 결합상수를 추정할 수 있었다.

• 한국전산구조공학회논문집
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• 제31권2호
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• pp.115-120
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• 2018

본 논문에서는 PSC 거더의 긴장력을 계측하기 위한 EM 센싱 기법을 다양한 PS 텐던에 적용하기 위하여 PS 강종별 긴장력 변화에 따른 자기이력 모니터링 결과를 소개한다. PSC 교량의 성능평가에 있어 PS 텐던의 긴장력은 매우 중요한 인자이나 현재는 시공시 설계 긴장력의 도입 여부만을 검증하고 그 이후에는 긴장력 관리가 이루어지지 않는 실정이다. 이를 계측하기 위하여 EM 센서를 이용하여 긴장력을 계측하는 기법에 대한 연구가 이루어지고 있으나 PSC 거더에 사용되는 모든 PS 텐던에 대한 연구는 이루어지지 않았다. 이에 본 연구에서는 PSC 교량에 주로 사용되는 B, C, D종 PS 텐던에 대해 EM 센싱 기법을 적용하기 위하여 각 강종별 긴장력에 따른 자기 이력 변화를 모니터링하였다. 이를 위해 B종 12.7mm, C종 15.2mm, D종 15.2mm PS 텐던 시편에 50, 100, 150, 180kN의 긴장력을 도입하고 각 긴장력 단계마다 자기 이력 곡선을 EM 센서를 통하여 계측하였다. 계측 결과 각 긴장력 단계마다 그 투자율이 정량적으로 변화하는 것을 확인할 수 있었다. 특히 B, C 종의 경우 단면적이 달라 선형회귀분석식의 상수는 상이하지만 유사한 기울기를 가지고 변화하고 D종의 경우 다른 강종과 다른 기울기를 가지고 변화하는 것을 확인하였다.

• 대한전자공학회:학술대회논문집
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• 대한전자공학회 2004년도 하계종합학술대회 논문집(2)
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• pp.447-450
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• 2004

The modeling circuit becomes more important in developing various magnetic devices regarding the fact that the competitive architecture and circuitry should be developed simultaneously. In this paper, we introduce a modeling circuit for hysteresis characteristic of a magnetic device, which is a major characteristic in the spin dependent magnetic material. This transistor-level model is conspicuous in that it can be usefully embodied in real circuits rather than conventional SPICE models are only for simulations.

• Progress in Superconductivity
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• 제9권1호
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• pp.11-17
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• 2007

Magnetization studies have been carried out on $MgB_2$ polycrystalline samples in the temperature range of 5 - 44 K and in the magnetic field up to 7 Tesla. The critical current density was calculated from hysteresis loops using the Bean's critical state model, and the highest value of $J_c$ at 20 K was $2.7{\times}10^5\;A/cm^2$ at 2 Tesla. The hysteresis loops were carefully examined to determine the temperature and magnetic field range where flux jumps appeared. The first jump occurred typically at 1 Tesla. Due to the strong pinning, we observed the presence of flux jump below H = 1 Tesla at temperature below 30 K.

• 대한전기학회논문지
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• 제40권3호
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• pp.258-265
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• 1991

In this paper, perpendicular magnetic recording system which consists of a single pole head and a double layer medium has been analyzed by using 2D-finite element method and preisach model for describing hysteresis characteristics. To verify the validity of this method, we compare the calculated magnetic field intensity which is above the isolated transition of magnetization with scaled up experimental data published in reference [7]. The results show good agreements within 7% error bounds and it is therefore concluded that this method will be very useful to analyze perpendicularmagnetic recording system with hysteresis characteristics.

• 대한기계학회논문집A
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• 제27권2호
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• pp.255-261
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• 2003

It is advantageous to use NDE methods to assess the mechanical properties of materials since the conventional method is time-consuming and sometimes requires cutting of sample from the component. The NDE parameters such as ultrasonic velocity and attenuation, electric resistivity, and magnetic coercive force and remanance have been utilized to evaluate changes of material properties due to heat treatment condition. It has been found that changes of materials properties under quenched and tempered/PWHT treatments could not be detected using EMAT and Electrical resistivity methods. However, victors hardness and magnetic hysteresis loop decreased with heat treatment procedures. These results were obtained using 3Cr-lMo-0.25V steel. The magnetic parameters were found to be most sensitive to changes of material properties.

• Journal of Electrical Engineering and Technology
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• 제13권5호
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• pp.1901-1907
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• 2018

This paper is a study for accurate iron loss calculation of a cylindrical linear machine for free piston engine. This study presents that it is possible to accurately predict power loss in ferromagnetic laminations under magnetic flux by specially considering the dependence of hysteresis, classical, and excess loss components on the magnetic induction derivative. Significant iron loss in the armature core will not only compromise the machine efficiency, but may also result in excessive heating, which could lead to irreversible deterioration in the machine performance. Thus, correct prediction of power losses under a distorted flux waveform is therefore an important prerequisite to machine design, particularly when dealing with large apparatus where stringent efficiency standards are required. Finally, it will be discussed about the iron loss in various materials of cylindrical linear electric machine by geometric and electrical parameters. It will give elaborate information about the perfect design and design rules of cylindrical linear machine and in parallel tools for the calculation, simulation and design will be available.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2003년도 춘계학술대회 논문집 초전도 자성체 연구회
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• pp.55-58
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• 2003

FeMn based spin valves often consist of a NiFe/FeMn/NiFe trilayer structure. We have investigated the evolution of exchange bias at the bottom and top interfaces in the NiFe(5nm)/FeMn(x)/NiFe(5nm) trilayer structure as a function of FeMn thickness in the range 3 nm to 30 nm. The XRD results indicate (111) textured growth for NiFe and FeMn layers. The magnetization studies using VSM show two hysteresis loops corresponding to the bottom NiFe seed layer and top NiFe layers with greater bias for the bottom NiFe layer, for FeMn thickness equal to and above 5 nm. The larger exchange bias for the bottom seed layer is confirmed by the surface sensitive MOKE hysteresis loop measurements which show gradual weakening of the MOKE hysteresis loop for the bottom NiFe layer with increasing FeMn thickness. The observed large exchange bias in a spin valve structure is usually attributed to the pinning NiFe layer on top of the FeMn layer, even when a NiFe seed layer of a few nm thickness is present, whereas, in reality it may be arising from the bottom seed layer, as shown by the present study.

• Current Applied Physics
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• 제18권11호
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• pp.1240-1247
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• 2018

Magnetic hysteresis in Ni nanowire arrays grown by electrodeposition inside the pores of anodic alumina templates is studied as a function of temperature in the range between 5 K and 300 K. Nanowires with different diameters, aspect ratios, inter-wire distance in the array and surface condition (smooth and rough) are synthesized. These microstructure parameters are linked to the different free magnetic energy contributions determining coercivity and the controlling magnetization reversal mechanisms. Coercivity increases with temperature in arrays of nanowires with rough surfaces and small diameters -33 nm and 65 nm- when measured without removing the alumina template and/or the Al substrate. For thicker wires -200 nm in diameter and relatively smooth surfaces- measured without the Al substrate, coercivity decreases as temperature rises. These temperature dependences of magnetic hysteresis are described in terms of an effective magnetic anisotropy $K_a$, resulting from the interplay of magnetocrystalline, magnetoelastic and shape anisotropies, together with the magnetostatic interaction energy density between nanowires in the array. The experimentally determined coercive fields are compared with results of micromagnetic calculations, performed considering the magnetization reversal mode acting in each studied array and microstructure parameters. A method is proposed to roughly estimate the value of $K_a$ experimentally, from the hysteresis loops measured at different temperatures. These measured values are in agreement with theoretical calculations. The observed temperature dependence of coercivity does not arise from an intrinsic property of pure Ni but from the nanowires surface roughness and the way the array is measured, with or without the alumina template and/or the aluminum support.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2001년도 하계학술대회 논문집
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• pp.905-908
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• 2001

The microstructure and the magnetic properties of Mn-Zn ferrite, which were power loss and saturation magnetic flux density, were investigated as the function of the process before firing. The highest initial permeability and the lowest power loss were attained to the specimen with CaO 400 ppm as a resulted from the highest solubility to SiO$_2$and the creation of liquid phase which improved sintering. The biggest grain size, the highest saturation magnetic flux density and the lowest power loss, which was resulted from that the eddy current loss increased as grain size increased but the hysteresis loss much more decreased and the hysteresis loss strongly influenced on the total power loss rather than the eddy current loss, were obtained to the Mn-Zn ferrite added 2wt% PVA. The power loss was lowest and the saturation magnetic flux density was highest in case of 1 ton/$\textrm{cm}^2$ and the grain size was not influenced.