• 한국자기학회지
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• 제5권5호
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• pp.805-809
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• 1995

In order to widen the band-width of ferrite absorber, compositional effect on the complex permeability of Ni-Zn ferrite and the structure of grid absorber were studied. From the experimental results, we could determine the optimum composition composition of Ni-Zn ferrite and the structure of grid absorber. Also, we manufactured grid absorber and investigated its microwave absorbing characteristics. Calculation shows that the ferrite frid absorber suppresses reflection ${\leq}-20dB$ from 30 MHz to 700 MHz and the conventional ferrite tile absorber suppresses reflection ${\leq}20dB$ in the frequency range of 30 MHz-400 MHz. It was found that the microwave absorbing performance of the ferrite grid absorber was superior to the ferrite tile absorber.

• 자원리싸이클링
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• 제13권6호
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• pp.37-42
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• 2004

NiO, ZnO 조성이 다른 Ni-Cu-Zn 페라이트의 손실 분석을 실시했다. 손실, Ph는 측정 온도의 상승에 따라 감소해 100-120$^{\circ}C$ 근처에서 일정한 값을 얻었다. Pcv의 주파수의존성은 Pcv~f$^n$ 로 표현될 수 있는데, n은 1 MHz까지 일정했다. Pcv는 ZnO/NiO비가 증가함에 따라 감소한다. Pcv를 Hysteresis loss(Ph) 및 잔류손실(Pcv-Ph)로 분리했다. Pcv의 온도특성 및 조성 의존성은 Ph에 기인하지만, Pcv-Ph는 온도 및 조성에 의존하지 않는다. Ph와 초투자율, ${\mu}_i$의 온도 및 조성 의존성을 분석해, 다음과 같은 식이 성립된다는 것을 알 수 있었다. ${\mu}_i{\mu}_0=I_s^2/(K_I+b{\sigma}_0{\lambda}_s)$ Wh=13.5(I$_s^2/{\mu}_i{\mu}_0)$ 여기서, ${\mu}_0$은 진공의 투자율, I$_s$는 포화자화, K$_I$는 이방성상수, ${\sigma}_0$는 내부 불균일 응력, ${\lambda}_s$는 자기이방성 상수, b는 미지의 상수, Wh는 1주기 당의 히스테리시스 손실(Ph=Wh${\times}$f)이다. Ni-Cu-Zn 페라이트의 Steinmetz 상수 m=1.64~2.2는 Mn-Zn 페라이트보다는 적은데, 이는 양 재료 간의 손실 메커니즘의 차가 있음을 암시하는 것이다.

• 한국표면공학회:학술대회논문집
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• 한국표면공학회 2012년도 춘계학술발표회 논문집
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• pp.256-256
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• 2012

SoP용 재료에 응용하기 위하여 NiCuZn 페라이트계 이용한 이종접합의 관한연구를 하였다. NiCuZn 페라이트계와 유전체의 이종접합특성은 XRD, Dilatometer, LCR meter, FE-SEM, EDS 이용하여 물리 화학적 특성을 조사하였다. NiCuZn 페라이트계는 일반적인 세라믹 제조공정을 이용하여 분말을 제조하였으며, 이종접합은 모든 시편에서 잘 진행되었으며 일부 유전체의 이온들이 페라이트 쪽으로 확산이 진행되었으며 NCZF700계는 $900^{\circ}C$ 소결 시편에서 확산이 진행되지 않은 현상이 나타났다.

• Journal of Magnetics
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• 제21권3호
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• pp.308-314
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• 2016

Cobalt-, zinc-, and nickel-zinc-substituted nano-size manganese ferrite powders, $MnFe_2O_4$, $Mn_{0.8}Co_{0.2}Fe_2O_4$, $Mn_{0.8}Zn_{0.2}Fe_2O_4$ and $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$, were fabricated using a sol-gel method, and their crystallographic and magnetic properties were subsequently studied. The $MnFe_2O_4$ ferrite powder annealed at temperatures above 523 K exhibited a spinel structure, and the particle size increased as the annealing temperature increased. All ferrites annealed at 773 K showed a single spinel structure, and the lattice constants and particle size decreased with the substitution of Co, Zn, and Ni-Zn. The $M{\ddot{o}}ssbauer$ spectrum of the $MnFe_2O_4$ ferrite powder annealed at 523 K only showed a doublet due to its superparamagnetic phase, and the $M{\ddot{o}}ssbauer$ spectra of the $MnFe_2O_4$, $Mn_{0.8}Co_{0.2}Fe_2O_4$, and $Mn_{0.8}Zn_{0.2}Fe_2O_4$ ferrite powders annealed at 773 K could be fitted as the superposition of two Zeeman sextets due to the tetrahedral and octahedral sites of the $Fe^{3+}$ ions. However, the $M{\ddot{o}}ssbauer$ spectrum of the $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$ ferrite powder annealed at 773 K consisted of two Zeeman sextets and one quadrupole doublet due to its ferrimagnetic and paramagnetic behavior. The area ratio of the $M{\ddot{o}}ssbauer$ spectra could be used to determine the cation distribution equation, and we also explained the variation in the $M{\ddot{o}}ssbauer$ parameters by using this cation distribution equation, the superexchange interaction and the particle size. Relative to pure $MnFe_2O_4$, the saturation magnetizations and coercivities were larger in $Mn_{0.8}Co_{0.2}Fe_2O_4$ and smaller in $Mn_{0.8}Zn_{0.2}Fe_2O_4$, and $Mn_{0.8}Ni_{0.1}Zn_{0.1}Fe_2O_4$. These variations could be explained using the site distribution equations, particle sizes and magnetic moments of the substituted ions.

• 한국재료학회지
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• 제16권9호
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• pp.578-583
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• 2006

We studied the physical properties of Ni-Zn ferrites by adding different chemicals such as $SO_4$, Cl, and $NO_3$. Specimens were prepared by the coprecipitation method and sintered at temperatures $950^{\circ}C,\;1,150^{\circ}C,\;and\;1,350^{\circ}C$, respectively. X-ray diffractions showed a spinel structure and the optical microscopy revealed grain size of 0.3 to 0.6 ${\mu}m$. The optimum sintering temperature to obtain fine, sintered microstructure depended on the additive : Cl and $NO_3\;at\;950^{\circ}C\;and\;SO_4\;at\;1,150^{\circ}C$. According to particle size analysis, higher magnetic permeability and magnetization value were observed with Cl and $NO_3\;than\;SO_4$. As sintering temperature was raised from $950^{\circ}C$ to $1,350^{\circ}C$, the average grain diameter, initial permeability and the magnetic moment also increased.

• 한국재료학회지
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• 제12권10호
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• pp.791-795
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• 2002

We studied the physical properties of $Co_3$$O_4$-added Ni-Zn ferrite which were sintered at 1050~110$0^{\circ}C$ for 2 hours. X-ray diffraction showed a spinel structure, and optical microscopy showed grain sizes of 5 to 10 $\mu\textrm{m}$. As the sintering temperature was increased from $1050^{\circ}C$ to $1070^{\circ}C$, the initial permeability and magnetic induction increased, and both of the loss factor and the coercive force decreased. The Curie temperatures were about $^234~245{\circ}C$ with added $Co_3$$O_4$. The initial permeability was 350 to 420 and maximum magnetic induction density and coercive force 4870G to 4980G and 0.15 Oe to 0.21 Oe, respectively which were similar to those of Ni-Zn ferrite synthesized in the conventional process. The frequency of specimen was in the range of 1MHz to 300MHz. In the plot of initial permeability vs. frequencies, a $180^{\circ}C$ rotation of the magnetic domain could be perceived in a broad band of microwave before and after the resonance frequency.

• 한국정보통신학회:학술대회논문집
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• 한국해양정보통신학회 2000년도 춘계종합학술대회
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• pp.160-164
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• 2000

본 연구에서는 전파흡수체용 Ferrite-Rubber Composite에서 Ferrite의 함량과 Composite의 전파흡수특성과의 상관관계에 관하여 알아보았다. 이때 Ferrite는 스피넬 구조의 형성과 결정입의 비교적 큰 성장을 위하여 $1200^{\circ}C$에서 2시간 열처리하여 제조한 시료를 사용하였다. $1200^{\circ}C$에서 열처리된 Ferrite를 사용한 Composite는 Ferrite 함량이 52 wt.%에서 57 wt.%로 증가하면 정합주파수는 변화는 없으며, 반사감쇠량이 증대되며, 62 wt.%인 경우, 정합주파수의 이동현상이 발생됨을 알 수 있었다. 이로부터 전파흡수체용 Ferrite-Rubber Composite에서 Ferrite 함량을 제어하므로써 Composite의 전파흡수특성을 제어하는 것이 가능하다는 것을 알 수 있었다.

• 한국세라믹학회지
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• 제28권7호
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• pp.556-560
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• 1991

The behavior of Ni-Zn ferrite/Mn-Zn ferrite composite electromagnetic absorber was investigated. The imaginary part of complex permeability of the composite was higher than that of either ferrite alone at all frequency range (50∼1400MHz) studied. The difference, which was pronounced in low frequency range, was reached the maximum value when the composite consisted of constituent ferrites with equal amount. Since the thickness in inversely proportional to the imaginary part of complex permeability for the ferrite absorber, it was possible to reduce the thickness of electromagnetic absorber by employing a composite of two different ferrites.

• 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.

• Journal of electromagnetic engineering and science
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• 제16권3호
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• pp.150-158
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• 2016

This paper reports on a study of LiNiZn-ferrite composite as a radiation absorbent material (RAM). The electromagnetic (EM) wave absorbers are composed of an EM wave absorbing material and a polymeric binder. The surface morphology, chemical composition, weight percent of the ferrite composite of the toroid sample, magnetic properties, and return loss are investigated using field emission scanning electron microscopy (FE-SEM), energy dispersive X-ray spectroscopy (EDX), X-ray photoelectron spectroscopy (XPS), thermogravimetric analysis (TGA), vibrating sample magnetometer (VSM), and network analyzer. For preparing the absorbing sheet, chlorinated polyethylene (CPE) is used as a polymeric binder. The EM wave absorption properties of the prepared samples were studied at 4 - 8 GHz. We can confirm the effects of the thickness of the samples for absorption properties. An absorption bandwidth of more than a 10-dB return loss shifts toward a lower frequency range along with an increase in the thickness of the absorber.