• Title/Summary/Keyword: 자기포화

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Magenetic Properties of Co, Ni and Ca Substituted Mn-Zn Ferrite (Co, Ni 및 Ca를 첨가한 Mn-Zn 페라이트의 자기적 성질)

  • 하태욱;이정식
    • Journal of the Korean Magnetics Society
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    • v.5 no.1
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    • pp.15-20
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    • 1995
  • We have prepared 20 kinds of Mn-Zn ferrites as content of CaO(0.1 mol%), NiO(0.0~0.60 mol%) and CoO(0.0~0.8 mol%) adding by the coprecipitation method and studied the magnetic properties as content of CaO, NiO and CoO adding. Initial permeability decrease as the content of NiO and CoO adding increases, while Curie tem~ perature increase as the content of NiO and CoO adding increases. $(H_{c})$, $(B_{s})$ and $(W_{h})$ increase as content of NiO adding increases.

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Crystall ographic and Magnetic Properties of Ultrafine $CoFe_{1.9}Bi_{0.1}O_4$ Grown by Using a Sol-Gel Method (Sol-gel법에 의한 초미세 분말 $CoFe_{1.9}Bi_{0.1}O_4$의 결정학적 및 자기적 성질 연구)

  • 김우철;김삼진;김철성;이승화
    • Journal of the Korean Magnetics Society
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    • v.9 no.4
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    • pp.177-183
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    • 1999
  • Ultrafine $CoFe_{1.9}Bi_{0.1}O_4$ particles were fabricated by using a sol-gel method and their magnetic and structural properties were investigated with an x-ray diffractometer (XRD), a vibrating sample magnetometer (VSM), and a M$\"{o}$ssbauer spectrometer. The result of x-ray diffraction and M$\"{o}$ssbauer spectroscopy showed that the powders fired at and above 523 K had only cubic spinel structures. M$\"{o}$ssbauer spectra measurements showed that the powders annealed at 523,723 and 823 K possessed ferrimagnetic nature and paramagnetic nature due to superparamagnetism, simultaneously at room temperature and the powders annealed at and above 923 K behaved ferrimagnetically. In the case of the powder annealed at 923 K, the lattice constant was $a_0=8.398$\pm$0.005{\AA}$ and the hyperfine fields were $H_{hf}(A)=479kOe,\; H_{hf}(B)=502kOe$. The isomer shifts indicate that the iron ions are ferric at tetrahedral[A] and octahedral sites [B], respectively. The magnetization as a function of annealing temperature increased as increasing annealing temperature. The largest coercivity values were $H_C=1368\;Oe$ AT 923 K annealing temperature. In the case of the powder annealed at 1123 K, the magnetization value was $M_S=75\;emu/g$ and this value was similler to that of $CoFe_2O_4$.Fe_2O_4$.

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Magnetic Properties of Ni Nanostructures Made by using Nanoporous Anodic Alumina (AAO를 이용한 Ni 나노구조체의 자기적 특징)

  • Lee, S.G.;Shin, S.W.;Lee, J.;Lee, J.H.;Kim, T.G.;Song, J.H.
    • Journal of the Korean Magnetics Society
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    • v.14 no.3
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    • pp.105-108
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    • 2004
  • Array of magnetic Ni nanostructures has been fabricated on Si substrate by using nanoporous alumina film as a mask during deposition. The nanostructures are truncated cone-shape and the lateral sizes are comparable to height. While the continuous film shows well-defined in-plane magnetization, the nanostructure shows perpendicular component of magnetization at remanence. The hysterectic behavior of nanostructures is dominated by the demagnetizing field instead of interaction among them.

Thickness Dependence of Amorphous CoSiB/Pd Multilayer with Perpendicular Magnetic Anisotropy (비정질 강자성체 CoSiB/Pd 다층박막의 두께에 따른 수직자기이방성 변화)

  • Yim, H.I.
    • Journal of the Korean Magnetics Society
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    • v.23 no.4
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    • pp.122-125
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    • 2013
  • Perpendicular magnetic anisotropy (PMA) is the phenomenon of magnetic thin film which is preferentially magnetized in a direction perpendicular to the film's plane. Amorphous multilayer with PMA has been studied as the good candidate to realization of high density STT-MRAM (Spin Transfer Torque-Magnetic Random Access Memory). The current issue of high density STT-MRAM is a decrease in the switching current of the device and an application of amorphous materials which are most suitable devices. The amorphous ferromagnetic material has low saturated magnetization, low coercivity and high thermal stability. In this study, we presented amorphous ferromagnetic multilayer that consists of an amorphous alloy CoSiB and a nonmagnetic material Pd. We investigated the change of PMA of the $[CoSiB\;t_{CoSiB}/Pd\;1.3nm]_5$ multilayer ($t_{CoSiB}$ = 0.1, 0.2, 0.3, 0.4, 0.5, 0.6 nm, and $t_{Pd}$ = 1.0, 1.1, 1.2, 1.3, 1.4, 1.5, 1.6 nm) and $[CoSiB\;0.3nm/Pd\;1.3nm]_n$ multilayer (n = 3, 5, 7, 9, 11, 13). This multilayer is measured by VSM (Vibrating Sample Magnetometer) and analyzed magnetic properties like a coercivity ($H_c$) and a magnetization ($M_s$). The coercivity in the $[CoSiB\;t_{CoSiB}\;nm/Pd\;1.3nm]_5$ multi-layers increased with increasing $t_{CoSiB}$ to reach a maximum at $t_{CoSiB}$ = 0.3 nm and then decreased for $t_{CoSiB}$ > 0.3 nm. The lowest saturated magnetization of $0.26emu/cm^3$ was obtained in the $[CoSiB\;0.3nm/Pd\;1.3nm]_3$ multilayer whereas the highest coercivity of 0.26 kOe was obtained in the $[CoSiB\;0.3nm/Pd\;1.3nm]_5$ mutilayer. Additional Pd layers did not contribute to the perpendicular magnetic anisotropy. The single domain structure evolved in to a striped multi-domain structure as the bilayer repetition number n was increased above 7 after which (n > 7) the hysteresis loops had a bow-tie shapes.

Development of Magnetic Torquer for Satellite Attitude Control (인공위성 자세제어용 Magnetic Torquer 개발)

  • Son, D.
    • Journal of the Korean Magnetics Society
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    • v.18 no.2
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    • pp.54-57
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    • 2008
  • Magnetic torquer, which uses torque between magnetic dipole moment and earth magnetic field, has been used to control attitude of satellites. In this work, we developed a magnetic torquer for small scientific satellite and test under environmental conditions of the satellite launching and orbital motion have been carried out. The developed magnetic torquer shows saturation magnetic dipole moment of $15Am^2$, linearity of 0.3 % in the range of ${\pm}12Am^2$, mass of 0.46 kg, and power consumption of 1 Watt at magnetic dipole moment of $10Am^2$.

A Study on the Microstructures and Magnetic Properties (Fe-(BN, Sin)박막의 미세구조와 자기특성에 관한 연구)

  • 신동훈;이창호;안동훈;남승의;김형준
    • Journal of the Korean Magnetics Society
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    • v.8 no.3
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    • pp.138-143
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    • 1998
  • We have investigated the magnetic properties of FeBN and FeSiN films deposited by RF magnetron reactive sputtering system. It was investigated that the compositions of B, Si and N were the main factors influencing the soft magnetic properties and film resistivity. The addition of small amount of N significantly improve the soft magnetic properties and electrical resistivity. The FeBN and FeSiN films were showed good soft magnetic properties which were Hc<1 Oe, Bs:19~19 kG and $\mu$'>1000 values. The composition of films were $Fe_{75}(BN)_{25},\;Fe_{78}(SiN)_{22}$ and resistivity was 100~120 $\mu$$\Omega$-cm. but, futher increase in B, Si and N concentration degraded the soft magnetic properties due to formation of nitride such as $Fe_4N$ compound.

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

  • 김덕실;조재경
    • Journal of the Korean Magnetics Society
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    • v.9 no.2
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    • pp.91-97
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    • 1999
  • YIG $(Y_3Fe_5O_{12})$ films with 4~80 ${\mu}{\textrm}{m}$ thickness were epitaxially grown on GGG $(Gd_3Ga_5O_{12})$ substrates by LPE (liquid phase epitaxy) techniques. Using various melts having different chemical composition the growth temperature was varied as a parameter. Growth rate, surface morphology, chemical composition, lattice constant, saturation magnetization, and magnetic resonance of the films were investigated. Lattice mismatch between the substrate and film Δa, saturation magnetization, and magnetic resonance line width ΔH increased, decreased, and increased, respectively, as undercooling temperature ΔT increased. The films grown by using the melt with larger R$_1$and smaller R$_3$had smaller ΔH. The major origin of the increase of ΔH was the increase of Δa. It is considered that the magnetic field in the film became locally inhomogeneous with the increase of Δa due to the increase of inhomogenity in stress distribution to the film depth direction. Therefore, in order to grow YIG films with small microwave loss it is necessary to grow films at small ΔT using the melt with large R$_1$and small R$_3$resulting in a small Δa.

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Effect of the Powder Characteristics of Iron Oxides on the Magnetic Properties of Sr-ferrite (산화철의 분체특성이 Sr-ferrite의 자기특성에 미치는 영향)

  • 조태식;김효준;최승덕;남효덕;염충진
    • Resources Recycling
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    • v.7 no.4
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    • pp.43-49
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    • 1998
  • We investigated the effects of the powder characteristics of various domestic iron oxides (${\alpha}Fe_2O_3$) on the magnetic properties of Sr-ferrites The particle size and the distribution of iron oxides were classified hy three different rerinning methods, and greatly a affected on the magn$\xi$tic prope$\pi$ies and the mmphology of Sr-ferntes. The agglomeration of Ruthner iron oxides and the large particles of Chemirite (CY) above $0.80{\mu}\textrm{m}$ were degraded the prope며es of Sr-fcrrites. The optimal magnetic prope$\pi$ies of Srt territes, showing 68.2 emu/g of saturation magnetization and 4300 Oe of intrinsic coerClvity, were achieved at the following c conditions; Chemirite (P2EP) iron oxides of $0.14{\mu}\textrm{m}$ molar ratio of 5.8. and calcination of $1150^{\circ}C$/1 hr.

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Vital Signs Investigation in Subjects Undergoing Magnetic Resonance Imaging (자기공명검사 시 활력 징후의 변화)

  • Jeong, Mi-Ae;Choi, Kwan-Woo
    • The Journal of the Korea Contents Association
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    • v.19 no.6
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    • pp.412-417
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    • 2019
  • This study was proposed to investigate vital signs in subjects undergoing high magnetic field (3T) MR imaging for provide basic data on causes of claustrophobia as few previous studies were conducted on this special issue. Vital signs of 104 patients were monitored before and during the clinically indicated MR examinations to identify any relationship between MR scanning and the vital signs. An increase of systolic, diastolic blood pressure and pulse pressure were observed. However, they were not statistically significant(p>0.05), which meant the vital signs measured before and during the MRI scanning showed no significant change. This study is considered to be meaningful basic data for analyzing the links between vital sign fluctuations on claustrophobia during routine clinical MR examinations.

Magnetic Properties of Zn and La-Zn Substituted Strontium Ferrite (Zn 및 La-Zn 치환에 따른 Sr 페라이트의 자기적 특성에 관한 연구)

  • 장세동;김종오;김종희
    • Journal of the Korean Magnetics Society
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    • v.11 no.6
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    • pp.256-261
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    • 2001
  • These experiments were carried out to examine the effects of element substitution of Zn and La-Zn for Sr-ferrite. The calcined properties of Zn and La-Zn element substitution were examined, and also the sintered magnetic properties were compared with the stoichiometric condition. The magnetization properties of calcined SrM materials is as follows; M$\_$s/ : 61.06 emu/g. Also, the magnetization properties of calcined Zn$\_$0.3/-SrM materials is as follows; M$\_$s/ : 66.90 emu/g. The sintered magnetic properties of (La-Zn)$\_$0.3/-SrM composition is as follows; B$\_$r/ : 4.21 kG, BH$\_$max/: 4.19 MGOe.

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