• 제목/요약/키워드: saturation magnetization

검색결과 467건 처리시간 0.028초

The Properties of Mn, Ni, and Al Doped Cobalt Ferrites Grown by Sol-Gel Method

  • Choi, Seung Han
    • 한국재료학회지
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    • 제28권7호
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    • pp.371-375
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    • 2018
  • The manganese-, nickel-, and aluminum-doped cobalt ferrite powders, $Mn_{0.2}Co_{0.8}Fe_2O_4$, $Ni_{0.2}Co_{0.8}Fe_2O_4$, and $Al_{0.2}CoFe_{1.8}O_4$, are fabricated by the sol-gel method, and the crystallographic and magnetic properties of the powders are studied in comparison with those of $CoFe_2O_4$. All the ferrite powders are nano-sized and have a single spinel structure with the lattice constant increasing in $Mn_{0.2}Co_{0.8}Fe_2O_4$ but decreasing in $Ni_{0.2}Co_{0.8}Fe_2O_4$ and $Al_{0.2}CoFe_{1.8}O_4$. All the $M{\ddot{o}}ssbauer$ spectra are fitted as a superposition of two Zeeman sextets due to the tetrahedral and octahedral sites of the $Fe^{3+}$ ions. The values of the magnetic hyperfine fields of $Ni_{0.2}Co_{0.8}Fe_2O_4$ are somewhat increased in the A and B sites, while those of $Mn_{0.2}Co_{0.8}Fe_2O_4$ and $Al_{0.2}CoFe_{1.8}O_4$ are decreased. The variation of $M{\ddot{o}}ssbauer$ parameters is explained using the cation distribution equation, superexchange interaction and particle size. The hysteresis curves of the ferrite powders reveal a typical soft ferrite pattern. The variation in the values of saturation magnetization and coercivity are explained in terms of the site distributions, particle sizes and the spin magnetic moments of the doped ions.

Post Annealing Effects on Iron Oxide Nanoparticles Synthesized by Novel Hydrothermal Process

  • Kim, Ki-Chul;Kim, Young-Sung
    • Journal of Magnetics
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    • 제15권4호
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    • pp.179-184
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    • 2010
  • We have investigated the effects of post annealing on iron oxide nanoparticles synthesized by the novel hydrothermal synthesis method with the $FeSO_4{\cdot}7H_2O$. To investigate the post annealing effect, the as-synthesized iron oxide nanoparticles were annealed at different temperatures in a vacuum chamber. The morphological, structural and magnetic properties of the iron oxide nanoparticles were investigated with high resolution X-ray powder diffraction (XRD), high resolution transmission electron microscopy (HRTEM), Mossbauer spectroscopy, and vibrating sample magnetometer analysis. According to the XRD and HRTEM analysis results, as-synthesized iron oxide nanoparticles were only magnetite ($Fe_3O_4$) phase with face-centered cubic structure but post annealed iron oxide nanoparticles at $700^{\circ}C$ were mainly magnetite phase with trivial maghemite ($\gamma-Fe_2O_3$) phase which was induced in the post annealing treatment. The crystallinity of the iron oxide nanoparticles is enhanced by the post annealing treatment. The particle size of the as-synthesized iron oxide nanoparticles was about 5 nm and the particle shape was almost spherical. But the particle size of the post annealed iron oxide nanoparticles at $700^{\circ}C$ was around 25 nm and the particle shape was spherical and irregular. The as-synthesized iron oxide nanoparticles showed superparamagnetic behavior, but post annealed iron oxide nanoparticles at $700^{\circ}C$ did not show superparamagnetic behavior due to the increase of particle size by post annealing treatment. The saturation of magnetization of the as-synthesized nanoparticles, post annealed nanoparticles at $500^{\circ}C$, and post annealed nanoparticles at $700^{\circ}C$ was found to be 3.7 emu/g, 6.1 emu/g, and 7.5 emu/g, respectively. The much smaller saturation magnetization value than one of bulk magnetite can be attributed to spin disorder and/or spin canting, spin pinning at the nanoparticle surface.

칩인덕터용 저온소성 Nano-glass 연구 (Low Firing Temperature Nano-glass for Multilayer Chip Inductors)

  • 안성용;위성권
    • 한국자기학회지
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    • 제18권1호
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    • pp.43-47
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    • 2008
  • [ $ZnO-Bi_2O_3-Al_2O_3-B_2O_3-SiO_2$ ] nano-glass를 sol-gel 법으로 제조 하였다. 평균 입자 크기는 60.3 nm였으며 매우 균일한 입도 분포를 가졌다. Nano-glass를 NiZnCu ferrite의 저온소성용 소결조제로 사용하였으며 NiZnCu ferrite에 nano-glass를 첨가한 후 $840{\sim}900^{\circ}C$에서 2시간 소결을 진행하였다. 소결성 및 자기적 특성에 대해 연구하였으며 밀도, 수축율, 초투자율, 품질계수, 및 포 화자화값을 측정하였다. nano-glass를 0.5 wt% 첨가하여 $900^{\circ}C$에서 소결한 토로이달 core 시편의 초투자율은 1 MHz에서 측정 시 193.3의 값을 가졌다. 초투자율과 포화자화값은 소결온도가 증가함에 따라 증가하는 경향을 나타내었다. sol-gel 법에 의해 제조된 $ZnO-Bi_2O_3-Al_2O_3-B_2O_3-SiO_2$ nano-glass를 칩인덕터용 NiZnCu ferrite의 저온 소결조제로 사용 가능함을 알 수 있었다.

마이크로파 소자용 에피틱시 YIG막의 성장과 특성 (Growth and Characterization of Epitaxial YIG Films for Microwave Devices)

  • 김덕실;조재경
    • 한국자기학회지
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    • 제9권2호
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    • pp.91-97
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    • 1999
  • 막후 4~80$\mu\textrm{m}$의 YIG(Y3FeO12)막을 GGG(Gd3Ga5O12) 기판 상에 수 종류의 화학조성이 서로 다른 Melt를 사용하여 성장 온도를 변화시키며 LPE(Liquid Phase Epitaxy)법으로 에피탁시 성장시켰다. 제조한 막의 성장속도, 표면 형상, 화학 조성, 격자상수, 포화 자화, 자기공명특성을 조사했다. 기판과 막간의 격자상수의 mismatch Δa, 포화자화 그리고 자기공명흡수반치폭 ΔH는 과냉각온도 ΔT가 증가함에 따라 각각 증가, 감소 및 증가하는 경향을 보였다. 또한, R1값이 작은 Melt를 사용한 경우, 동일한 Δa가 증가하면 막후 방향으로의 응력 분포가 불균일해져 막 내부의 자장이 불균일해지기 때문으로 생각된다. 따라서, 마이크로파 손실이 작은 양질의 마이크로파 소자용 YIG막을 제조하기 위해서는 R1값이 크고 R3값이 작은 Melt를 사용하여 ΔT가 작은 영역에서 막을 성장시켜 ΔT가 작은 영역에서 막을 성장시켜 Δa를 작게 해야만 한다.

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YIG ($Y_3$$Fe_5$O_{12}$)의 미세구조 및 자성 특성에 대한 $SrTiO_3$첨가 영향 (The Effects of $SrTiO_3$ Addition on the Microstructure and Magnetic Properties of YIG)

  • 장학진;윤석영;김태옥
    • 한국재료학회지
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    • 제11권3호
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    • pp.203-206
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    • 2001
  • SrTiO$_3$첨가량 및 소결온도에 따른 YIG 소결체의 미세구조 및 자기적 특성변화에 대하여 조사하였다. 소량의 SrTiO$_3$소결재를 첨가한 결과 소결체의 격자상수는 약간 증가하였으며, 이는 소결시 $Y^{+3}$, Fe$^{+3}$이온이 이온반경이 상대적으로 큰 Sr$^{+2}$, Ti$^{+4}$이온으로 치환되었기 때문인 것으로 추정된다. SrTiO$_3$소결재를 0.2mo1% 첨가하고, 142$0^{\circ}C$에서 소결한 소결체의 밀도는 이론밀도의 98%이상의 치밀화를 얻을 수 있었다. 상온에서의 포화자화값(M$_s$)은 SrTiO$_3$소결재의 첨가량이 증가함에 따라 약간 감소하였으나 큰 변화는 없었다. 더욱이 온도에 따른 보자력 (H$_c$)의 변화는 없었다.

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Effects of Ga Substitution on Crystallographic and Magnetic Properties of Co Ferrites

  • Chae, Kwang Pyo;Choi, Won-Ok;Kang, Byung-Sub;Lee, Young Bae
    • 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.

자기포화를 이용한 강자성체의 와전류검사장비 개발 (Development of Eddy Current Testing System using Magnetic Saturation in ferromagnetic Materials)

  • 성제중;신용훈;엄태건;강석철;권영호;서동만
    • 비파괴검사학회지
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    • 제23권4호
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    • pp.356-363
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    • 2003
  • 플랜트, 산업용 설비로서 사용되어지고 있는 강관의 결함 검출을 위한 와전류검사장비를 개발하였다. 강관은 내부 불균일 한 전자기적 특성을 포함하고 있는 자성체로서 와전류검사의 응답신호를 왜곡시키므로 이러한 전자기적 특성의 균일화를 위해 자기포화가 요구된다. 자기포화가 없을 경우 결함신호는 잡음신호와 구별되지 않았으나 약 0.62A의 전류가 코일에 가해졌을 때 자기포화되어 결함을 검출 할 수 있었다 자기포화형 탐촉자는 헬름홀츠 코일을 적용하여 제작하였고 내부 대역 통과필터를 이용하여 직류자기장으로 야기되는 잡음신호를 최소화하였다. 개발된 장비를 이용한 현장실험 결과 1m/sec의 이송속도에서 관통홀$({\phi}=2.0mm)$ 결함을 정확히 검출 할 수 있었다.

유기금속 전구체로부터 초미립 $Fe_2O_3$ 분말의 저온 합성 (Low-Temperature Preparation of Ultrafine Fe2O3 Powder from Organometallic Precursors)

  • 김정수;김익범;강한철;홍양기
    • 한국세라믹학회지
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    • 제29권12호
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    • pp.942-948
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    • 1992
  • Ultrafine iron oxide powder, {{{{ gamma }}-Fe2O3 and $\alpha$-Fe2O3, were prepared by the thermal decomposition of organometallic compounds. The formation process of powder includes the thermal decomposition and oxidation of the organometallic precursors, Fe(N2H3COO)2(N2H4)2 (A) and N2H5Fe(N2H3COO)3.H2O (B). The organometallic precursors, A and B, were synthesized by the reaction of ferrous ion with hydrazinocarboxylic acid, and characterized by quantitative analysis and infrared spectroscopy. The mechanistic study for the thermal decomposition was performed by DAT-TG. The iron oxide powder was obtained by the heat treatment of the precursors at 20$0^{\circ}C$ and $600^{\circ}C$ for half an hour in air. The phases of the resulting product were proved {{{{ gamma }}-Fe2O3 and $\alpha$-Fe2O3 respectively. The particle shape was equiaxial and the particle size was less than 0.1 ${\mu}{\textrm}{m}$. Magnetic properties of the {{{{ gamma }}-Fe2O3 powder obtained from A and B was 234 Oe of coercivity, 64.26 emu/g of saturation magnetization, 23.59 emu/g of remanent magnetization and 24.1 Oe, 47.27 emu/g, 3.118 emu/g respectively. The value of $\alpha$-Fe2O3 powder was 1.494 Oe, 0.4862 emu/g, 0.1832 emu/g and 1,276 Oe, 0.4854 emu/g, 0.1856 emu/g respectively.

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Chemical Leaching of Non-Equilibrium Al(Fe-Co) Powder Produced by Rod Milling

  • Kim, Hyun-Goo
    • 한국분말재료학회지
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    • 제10권5호
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    • pp.305-309
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    • 2003
  • We report on the formation and chemical leaching of non-equilibrium $Al_{0.6}(Fe_{75}Co_{25})$ alloy produced by rod milling. X-ray diffractometry, transmission electron microscopy, differential scanning calorimetry, scanning electron microscopy, and vibrating sample magnetometry were used to characterize the as-milled and leached specimens. After 400 h, only the $Al_{0.4}Fe_{0.6}$ peak of the body-centered cubic type was present in the XRD pattern. The entire rod milling process could be divided into three different stages of milling: agglomeration, disintegration, and homogenization. The saturation magnetization, $M_s$ decreased with increased milling time, the $M_s$ of the powders before milling was about 113.8 emu/g, the $M_s$ after milling for 400 h was about 11.55 emu/g. Leaching of the Al in KOH of the Al at room temperature from the as-milled powders did not induce any significant change in the diffraction pattern. After the leached specimen had been annealed at $600^{\circ}C$ for 1 hour, the nanoscale crystalline phases were transformed into the bcc Fe, cubic Co, and $CoFe_2O_4$ phases. On cooling the specimen from 85$0^{\circ}C$, the degree of magnetization increased slightly, then increased sharply at approximately 364.8$^{\circ}C$, indicating that the bcc $Al_{0.4}Fe_{0.6}$ phase had been transformed to the Fe and Co phases.

$(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ 화합물의 구조 및 자기특성 (Structure and Magnetic Properties of $(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ Compounds)

  • 김희태;김윤배;김창석;김택기;권혁무
    • 한국자기학회지
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    • 제3권3호
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    • pp.196-200
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    • 1993
  • $(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ 화합물(RE=Ce, Pr, Nd, Sm, Gd, Tb, Dy)은 정방정(tetragonal) $ThMn_{12}$ 형 구조로 형성되며 c축을 자화용이축으로하는 일축결정자기이방성을 갖 는다. 주조한 $(Sm_{0.5}RE_{0.5})Fe_{11}Ti$ 화합물은 RE=Sm일 때 가장 높은 이방성자장 11200 kA/m(140 kOe)을 가지며, RE=Nd일 때 포화자화가 $122.3\;Am^{2}/kg$(122.3 emu/g)로 가장 크며, RE=Gd일 때 큐리온도가 $326^{\circ}C$로 가장 높다.

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