• 한국재료학회:학술대회논문집
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• 한국재료학회 2001년도 추계 학술발표강연 및 논문개요집
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• pp.17-17
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• 2001

• 한국결정성장학회지
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• 제22권5호
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• pp.218-222
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• 2012

FeNi alloy nanofibers have been prepared by an electrospinning process followed by air-calcination and H2 reduction to develop electromagnetic (EM) wave absorbers in the giga-hertz (GHz) frequency range. The thermal behavior and phase and morphology evolution in the synthetic processes were systematically investigated. Through the heat treatments of calcination and H2 reduction, as-spun PVP/FeNi precursor nanofiber has been stepwise transformed into nickel iron oxide and FeNi phases but the fibrous shape was maintained perfectly. The FeNi alloy nanofiber had the high aspect ratio and the average diameter of approximately 190 nm and primarily composed of FeNi nanocrystals with an average diameter of ~60 nm. The FeNi alloy nanofibers could be used for excellent EM wave absorbing materials in the GHz frequency range because the power loss of the FeNi nanofibers increased up to 20 GHz without a degradation and exhibited the superior EM wave absorption properties compared to commercial FeNi nanoparticles.

• 한국자기학회지
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• 제8권2호
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• pp.62-66
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• 1998

본 논문은 자기적 특성이 우수한 Ni-Zn-Cu ferrite를 얻기 위해 Bi2O3와 V2O5를 첨가하여 90$0^{\circ}C$에서 4시간 동안 소결한 후 각각의 시편에 대해서 물리적, 자기적 특성을 조사하였다. 큐리 온도는 Ni의 첨가량이 증가할수록 240~27$0^{\circ}C$까지 거의 직선적으로 증가하였다. 첨가제로 V2O5 와 Bi2O3를 사용한 경우 저온에서 소결을 가능하게 하여 최대 자속 밀도 Bm을 2650G에서 각각 3300G, 3500G로 높일수 있었으며 보자력은 2.05~1.05Oe까지 감소하였다. 첨가제로 V2O5와 Bi2O3를 사용한 경우 모두 투자율이 증가하였다. 상대 손실 계수는 Bi2O3를 첨가한 경우 입게의 비저항을 높여, 1 MHz의 주파수 대역에서 상대 손실 계수를 측정한 결과 6.3$\times$10-5~7.84$\times$10-5의 낮은 값을 얻었다. V2O5의 경우에는 투자율은 증가하였으나 Q값이 감소하여 상대 손실 계수가 증가하였다.

• 한국결정성장학회지
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• 제33권6호
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• pp.294-302
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• 2023

Ni-Mn-Zn ferrite, Ni_0.5-xMn_xZn_0.5Fe₂O₄(0 ≤ x ≤ 0.5)를 sol-gel 법으로 합성하여 Mn 치환량 x에 따른 결정 구조와 미세구조, 자기적 특성, 고주파 특성, 그리고 전자기파 흡수 특성을 연구하였다. Mn의 함량이 증가함에 따라 보자력 (H_C)에 큰 변화 없이 포화자화값(M_S)이 연속적으로 감소하는 것을 확인하였다. Ni-Mn-Zn ferrite-epoxy(10 wt%) 복합체에 대하여 0.1~18 GHz 주파수 범위에서 고주파 복소 유전율(ε', ε'') 및 복소 투자율(µ', µ'') spectra를 측정하고 전송선 이론을 통하여 전자기파 흡수 특성을 평가하였다. 각 시료는 1.5~2.5 GHz 및 6~11 GHz 범위에서 최소 반사손실 RL_min < -40 dB를 만족하는 1, 2차 강한 전자기파 흡수 영역이 존재하였고, Mn이 치환됨에 따라 RL_min 주파수는 저주파 방향으로 이동하였다. 또한 Ni-Zn ferrite(x = 0) 시료에 대하여 자기장(H)을 100 Oe에서 최대 400 Oe까지 단계적으로 인가한 상태로 ε', ε'', µ', µ'' spectra를 얻고 전자기파 흡수 특성을 평가하였다. 인가자장의 증가에 따라 시료의 강자성 공명 주파수가 증가하기 때문에 µ', µ'' spectra도 고주파 방향으로 단계적으로 이동해갔으며 최대 전자기파 흡수 주파수도 이에 대응하여 이동하였다. 이는 Ni-Mn-Zn ferrite에서 전자기파의 흡수는 자기적 손실에 의존하기 때문이며 Mn의 치환이나 인가자장에 의해 µ', µ'' spectra를 조절하면 전자기파 흡수 주파수도 조절할 수 있음을 보여준다. Ni-Zn ferrite-epoxy는 2.8~11.6 GHz에서 RL < -10 dB를 만족하는 광대역 전자기파 흡수 특성을 보였다.

• 한국전기전자재료학회논문지
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• 제27권7호
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• pp.462-467
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• 2014

In this paper, we studied the magnetic composite sheets for electromagnetic wave noise absorber of quasi-microwave band by using soft magnetic FeSiCr and Fe50Ni flakes with the thickness of about $1{\mu}m$ and polymer. The magnetic hysteresis curve including saturation magnetization and residual magnetization and the complex permeability characteristics of the composite sheets were investigated to clarify the mixing effect on electromagnetic wave absorption properties. The saturation magnetization was decreased about 10% while the residual magnetization was increased about 15% and the real parts of complex permeability at below 500 MHz were increased 0.6~4 while those values at above 500 MHz were decreased 0.4~2.5 according to the change of contents of FeSiCr and Fe50Ni powders. As a result, the reflection loss can be moved to the lower frequency from 2~3 GHz to 1~1.5 GHz as the contents of Fe50Ni flaky powder into FeSiCr flaky powder was increased up to 50%.

• 한국분말재료학회지
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• 제23권2호
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• pp.132-135
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• 2016

This study investigates the influence of sintering temperature on the magnetic properties and frequency dispersion of the complex permeability of Ni-Zn-Cu ferrites used for magnetic shielding in near-field communication (NFC) systems. Sintered specimens of $(Ni_{0.7}Zn_{0.3})_{0.96}Cu_{0.04}Fe_2O_4$ are prepared by conventional ceramic processing. The complex permeability is measured by an RF impedance analyzer in the range of 1 MHz to 1.8 GHz. The real and imaginary parts of the complex permeability depend sensitively on the sintering temperature, which is closely related to the microstructure, including grain size and pore distribution. In particular, internal pores within grains produced by rapid grain growth decrease the permeability and increase the magnetic loss at the operating frequency of NFC (13.56 MHz). At the optimized sintering temperature ($1225-1250^{\circ}C$), the highest permeability and lowest magnetic loss can be obtained.

• 열처리공학회지
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• 제19권5호
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• pp.249-256
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• 2006

Structural studies have been performed on precipitation hardening found in $L1_2$ ordered ${\gamma}^{\prime}-Ni_3(Al,Ti)$ alloys using transmission electron microscopy. A uniform solid solution of ${\gamma}^{\prime}-L1_2$ ordered phase supersaturated with Ni can be obtained by solution annealing in a suitable temperature range. The ${\gamma}^{\prime}$ phase hardens appreciably by the fine precipitation of disordered ${\gamma}$. The shape of ${\gamma}$ precipitates formed during aging is initially spherical or round-cubic and grow into platelets as aging proceeds. High resolution electron microscopy revealed that the ${\gamma}$ precipitates are perfectly coherent with the matrix ${\gamma}^{\prime}$ as long as the ${\gamma}$-precipitates are plates. The loss of coherency initiates by the introduction of dislocations at the ${\gamma}/{\gamma}^{\prime}$ interface followed by the step formation at the dislocations. The ${\gamma}$ precipitates become globular after the loss of coherency. The strength of ${\gamma}^{\prime}-Ni_3(Al,Ti)$ increases over the temperature range of experiment by the precipitation of fine ${\gamma}$ particles. The peak temperature where a maximum strength was obtained shifted to higher temperature.

• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2003년도 추계학술대회 논문집 Vol.16
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• pp.296-299
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• 2003

In this paper, $0.10Pb(Sb_{1/2}Sn_{1/2})O_3-0.25PbTiO_3-0.65PbZrO_3$ ceramics were fabricated by the mixed-oxide method. The sintering temperature and time were $1230^{\circ}C$ and 2[hr], respectively. The structural, dielectric and piezoelectric properties with addition of NiO were studied. The crystal structure of a specimen was rhombohedral. As a result of SEM, the average grain size were decreased with increasing the contents of NiO. But the grains of the specimens doped with 0.4wt% NiO were increased, due to deposits of excess NiO at grain boundaries in the liquid phase. Relative dielectric constant and dielectric loss of the specimen doped with 0.1wt% NiO were 701 and 0.026, respectively.

• 한국초전도ㆍ저온공학회논문지
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• 제23권4호
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• pp.44-48
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• 2021

In order to obtain ultra-high resolution MRI images, research and development of 11 T or higher superconducting magnets have been actively conducted in the world, recently. The high-temperature superconductor (HTS), first discovered in 1986, was very limited in industrial application until mid-2010, despite its high critical current characteristics in the high magnetic field compared to the low-temperature superconductor. This is because HTS magnets were unable to operate stably due to the thermal damage when a quench occurred. With the introduction of no-insulation (NI) HTS magnet winding technology that does not burn electrically, it could be expected that the HTS magnets are dramatically reduced in weight, volume, and cost. In this paper, a 6 T-class NI HTS magnet for basic characteristic analysis was designed, and a distributed equivalent circuit model of the NI coils was configured to analyze the charging current characteristics caused by excitation current, and the charge delay phenomenon and loss were predicted through the development of a simulation model. Additionally, the critical current of the NI HTS magnets was estimated, considering the magnetic field, its angle and temperature with a given current. The loss due to charging delay characteristics was analyzed and the result was shown. It is meaningful to obtain detailed operation technology to secure a stable operation protocol for a 6T NI HTS magnet which is actually manufactured.

• 한국분말재료학회지
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• 제26권2호
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• pp.107-111
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• 2019

The activation energy to create a phase transformation or for the reaction to move to the next stage in the milling process can be calculated from the slop of the DSC plot, obtained at the various heating rates for mechanically activated Al-Ni alloy systems by using Kissinger's equation. The mechanically activated material has been called "the driven material" as it creates new phases or intermetallic compounds of AlNi in Al-Ni alloy systems. The reaction time for phase transformation by milling can be calculated using the activation energy obtained from the above mentioned method and from the real required energy. The real required energy (activation energy) could be calculated by subtracting the loss energy from the total input energy (calculated input energy from electric motor). The loss energy and real required energy divided by the reaction time are considered the "metabolic energy" and "the effective input energy", respectively. The milling time for phase transformation at other Al-Co alloy systems from the calculated data of Al-Ni systems can be predicted accordingly.