• 한국자기학회지
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• 제20권5호
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• pp.182-186
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• 2010

Cobalt가 치환된 NiZnCu ferrite의 소결 및 자기적 성질에 미치는 영향에 대해 연구 하였다. 칩인덕터용 $Ni_{0.36-x}Co_xZn_{0.44}Cu_{0.22}Fe_{1.98}O_4(0{\leq}x{\leq}0.04)$를 고상반응법으로 제조하였다. 소결조제를 사용하지 않고 $880{\sim}920^{\circ}C$에서 공기중 2시간 열처리 하였으며 초투자율, 품질계수 Q, 밀도, 수축율, 포화자화, 및 보자력을 측정하였다. Cobalt가 치환된 NiZnCu ferrite는 품질계수 Q를 증가시켰으며 칩인덕터용으로 사용 가능함을 알 수 있었다. 품질계수 Q는 치환량이 x = 0.01까지 증가한 후 x = 0.01 이후로 급격히 감소하였다. Cobalt의 치환량이 증가함에 따라 초투자율 및 밀도값은 감소하였다. $900^{\circ}C$에서 소성된 $Ni_{0.35}Co_{0.01}Zn_{0.44}Cu_{0.22}Fe_{1.98}O_4$ 토로이달 core 샘플의 경우 1 MHz에서 측정 시 초투자율값은 130이었고 품질계수 Q값은 230으로 나타났다.

• 자원리싸이클링
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• 제2권2호
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• pp.9-15
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• 1993

본 연구에서는 광양제철소 전로 dust를 사용하여 자력산별 및 심강(분급) 실험을 통해서 산화철(magnetite)를 분리.회수하였다. 그리고 분리.회수한 산화철(magnetite)과 SrCO$_{#}$를 고상방응시켜 Sr-ferrite를 제조하고 그 자기적 특성은 조사하였으며, 이를 통하여 다음과 같은 결론을 얻었다. 1. 광양제철소 제동전로 Ep dust는 대부분 ${\alpha}$-Fe와 magnetite, wustite 등의 철산화물 상태로 존재하며 자력산별과 심강(분급)실험을 행한 결과 magnetite가 주된 구성물질인 산물을 얻을 수 있었다. 2. 전로 dust 정제를 통하여 얻어진 magnetite와 SrCO$_{4}$를 혼합한 후 하소를 행한 결과 magnetite의 산화배소과정 없이도 Sr-ferrite 생성이 가능함을 확인 하였으며, Sr-ferrite 생성 반응은 다음과 같다. I. $SrCO_3$ $+Fe_3$O$_4$+1/2(1-X)$O_2 $longrightarrow$\alpha$ $-Fe _2$$O_3$ $+SrFeO _3$\ulcorner+$CO_2$ II. $5.5\alpha$ $-Fe_2$$O_3$ $+SrFeO_3$\ulcornerlongrightarrowSrFe\ulcornerO\ulcorner+1/2(1/2-X)$O_2$ 3. 1150$^{\circ}C$에서 1시간동안 하소한 후 1250$^{\circ}C$에서 2시간 동안 산결하여 Br=3.75GK, $_{1}$Hc=1.7KOe, (B.H)$_{max}$=2.64 MGOe인 Sr-ferrite 이방성 영구자석을 제조하였다.

• Journal of Magnetics
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• 제20권1호
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• pp.26-30
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• 2015

The crystallographic and magnetic properties of gallium-substituted cobalt ferrite ($CoGa_xFe_{2-x}O_4$) were investigated. The new material was synthesized using conventional ceramic methods, with gallium substituted for ferrite in the range of x = 0.0 to 1.0, in steps of 0.2. X-ray diffraction and M$\ddot{o}$ssbauer spectroscopy were used to confirm the presence of crystallized particles in the $CoGa_xFe_{2-x}O_4$ ferrite powders. All of the samples exhibited a single phase with a spinel structure, and the lattice parameters decreased as the gallium content increased. The particle size of the samples also decreased as gallium increased. For $x{\leq}0.4$, the M$\ddot{o}$ssbauer spectra of $CoGa_xFe_{2-x}O_4$ could be fitted with two Zeeman sextets, which are the typical spinel ferrite spectra of $Fe^{3+}$ with A- and B-sites. However, for $x{\geq}0.6$, the M$\ddot{o}$ssbauer spectra could be fitted with two Zeeman sextets and one doublet. The variation in the M$\ddot{o}$ssbauer parameters and the absorption area ratio indicated a cation distribution of $(Co_{0.2-0.2x}Ga_xFe_{0.8-0.6x})[Co_{0.8+0.2x}Fe_{1.2-0.4x}]O_4$, and the magnetic behavior of the samples suggested that the increase in gallium content led to a decrease in the saturation magnetization and in the coercivity.

• 공업화학
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• 제30권1호
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• pp.54-61
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• 2019

본 연구에서는 Cu(II)의 흡착처리 후, 용액 내 함유된 폐흡착제의 효율적인 분리를 위하여 제올라이트(zeolite 4A)의 표면에 금속(Me = Co, Mn, Ni)이 치환된 페라이트 나노 입자를 성장시킨 자성흡착제를 합성하였다. 제올라이트 표면의 금속 페라이트는 용매열 합성법으로 제조되었으며, 자성흡착제의 특성은 XRD (X-ray diffractometer), SEM (scanning electron microscopy) 및 PPMS (physical property measurement system)로 분석하였다. Co-ferrite가 코팅된 제올라이트 복합체(CFZC)의 포화자화율이 5 emu/g으로 가장 높았으며, Cu(II)의 흡착 성능도 우수하였다. CFZC에 의한 Cu(II)의 흡착결과 값들은 298 K에서 Langmuir식에 잘 적용되었다. 그리고 Cu(II)의 흡착공정은 유사 2차 속도식에 부합하였다. 자유에너지 변화값(${\Delta}G^0=-4.63{\sim}-5.21kJ/mol$)은 Cu(II)의 흡착이 298~313 K 범위에서 자발적임을 나타내었다.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 1998년도 추계연구발표회 논문개요집
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• pp.64-65
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• 1998

• 한국자기학회지
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• 제5권5호
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• pp.800-804
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• 1995

The complex permeability dispersions and the microwave absorbing phenomena are investigated in ferrite microwave absorber. The complex permeability of NiZn ferrite, NiZnCo ferrite, and Y-type hexagonal ferrite were measured in 200MHz-14GHz range. Two types of resonances, the domain wall and the spin rotational resonance, were observed. With a ferrite particle with a diameter of about $1\;\mu\textrm{m}$, only spin rotational resonance were observed. The theoretical matching frequency is determined by plotting the measured complex permeability locus on the impedance matching solution map. One or two impedance matching phenomena are observed in the ferrite absorbers according to their complex permeability loci on the impedance matching solution map. The first matching frequency, found in the ferrite-rubber composites, which was higher than that of spin rotational resonance, increased with spin rotational resonance frequency.

• Journal of electromagnetic engineering and science
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• 제14권3호
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• pp.317-319
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• 2014

In this letter, a small-loop antenna for a mobile UHF RFID device is proposed. To achieve size reduction, a ferrite sheet optimized for a 900 MHz band is applied. The overall dimensions of the antenna are $46mm{\times}35mm{\times}0.24mm$, and it has a bandwidth of 45 MHz with a return loss of less than -6 dB. The proposed antenna satisfies near and far field UHF EPC global frequency band communications (902-928 MHz).

• 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.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2009년도 제40회 하계학술대회
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• pp.1293_1294
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• 2009

The sintering and high frequency electro-magnetic properties of Ba-hexagonal ferrite were investigated. All samples of the Ba-hexagonal ferrite were prepared by the conventional mixed oxide method and sintered at $1150^{\circ}C$~$1400^{\circ}C$. From the X-ray diffraction patterns of sintered Ba-hexagonal ferrite, the $Ba_3Co_2Fe_{24}O_{41}$ phase was represented as main phase in the almost sintering conditions. The bulk densities with sintering temperature and decreased at $1400^{\circ}C$. The permittivity ($\varepsilon$') and loss tangent of permittivity ($\varepsilon$"/$\varepsilon$') of $Ba_3Co_2Fe_{24}O_{41}$ ceramics increased and decreased with sintering temperature, respectively. The permeability of $Ba_3Co_2Fe_{24}O_{41}$ ceramics decreased with sinteirng temperature. The loss tangent of permeability was not changed compared each other with sintering temperature. The bulk density of $Ba_3Co_2Fe_{24}O_{41}$ ceramics sintered at $1300^{\circ}C$ was 4.79 g/$cm^3$. The permittivity, loss tangent of permittivity and permeability, loss tangent of permeability were 19.896, 0.1718 and 14.218, 0.2046 at 210 MHz, respectively.

• 한국세라믹학회지
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• 제20권4호
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• pp.340-346
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• 1983

The effect of aging coprecipitate obtained by the reaction of mixed solution 1.1 mol FeCl-0.1 mol $BaCl_2$ and 4.0 mol. NaOH-1.0 mol $K _2 CO_3$ on the synthesis process of Baferrite $(BaFe_{12}O_{19})$ was investigated by means of DTA, TGA, XRD and electron microscope. The no-aged coprecipitate seems to be the aggregate of amorphosus $Fe_3$ .$nH_2O$ and (1-X) $BaCO_3$.$xBa(OH)_2$, but the 30 days-aged to be composed of crystalline $Fe_2O_3H_2O$ and $BaCO_3$. The decomposition temperature of $BaCO_3$ in the coprecipitate increases from 400-$700^{\circ}C$ to 700-90$0^{\circ}C$ with increment of aging-time. In the no-aged coprecipitate Ba-ferrite is synthesized through the surface reaction of amorphous Fe_2O_3$ and skeleton crystal BaO at 800-90$0^{\circ}C$ with more compact crystalization. During calcination of the 30 days-aged coprecibitate the intermediate phase BaFe_2O_4$ is formed at 600-$700^{\circ}C$ and completely transformed to Ba-ferrite at 800-90$0^{\circ}C$.