• Journal of Magnetics
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• 제15권4호
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• pp.159-164
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• 2010

The Zn, Co and Ni substituted manganese ferrite powders, $Mn_{1-x}$(Zn, Co, Ni)$_xFe_2O_4$, were fabricated by the solgel method, and their crystallographic and magnetic properties were studied. The Zn substituted manganese ferrite, $Zn_{0.2}Mn_{0.8}Fe_2O_4$, had a single spinel structure above $400^{\circ}C$, and the size of the particles of the ferrite powder increased when the annealing temperature was increased. Above $500^{\circ}C$, all the $Mn_{1-x}$(Zn, Co, Ni)$_xFe_2O_4$ ferrite had a single spinel structure and the lattice constants decreased with an increasing substitution of Zn, Co, and Ni in $Mn_{1-x}$(Zn, Co, Ni)$_xFe_2O_4$. The Mossbauer spectra of $Mn_{1-x}Zn_xFe_2O_4$ (0.0$\leq$x$\leq$0.4) could be fitted as the superposition of two Zeeman sextets due to the tetrahedral and octahedral sites of the $Fe^{3+}$ ions. For x = 0.6 and 0.8 they showed two Zeeman sextets and a single quadrupole doublet, which indicated they were ferrimagnetic and paramagnetic. And for x = 1.0 spectrum showed a doublet due to a paramagnetic phase. For the Co and Ni substituted manganese ferrite powders, all the Mossbauer spectra could be fitted as the superposition of two Zeeman sextets due to the tetrahedral and octahedral sites of the $Fe^{3+}$ ions. The variation of the Mossbauer parameters are also discussed with substituted Zn, Co and Ni ions. The increment of the saturation magnetization up to x = 0.6 in $Mn_{1-x}Co_xFe_2O_4$ could be qualitatively explained using the site distribution and the spin magnetic moment of substituted ions. The saturation magnetization and coercivity of the $Mn_{1-x}$(Zn, Co, Ni)$_xFe_2O_4$ (x = 0.4) ferrite powders were also compared with pure $MnFe_2O_4$.

• 한국재료학회지
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• 제4권8호
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• pp.952-957
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• 1994

RF & DC magnetron sputtering장치를 이용하여 Ar과 $Ar+N_{2}$혼합가스분위기에서 Fe/Co및 Fe-N/Co-N다층막을 각각 제조하였다. 제작된 다층막을 $100^{\circ}C$ ~ $500^{\circ}C$로 각각 1시간씩 열처리하였다. Fe막의 두께와 열처리 온도에 따른 Fe/Co다층막의 포화자화와 보자력을 측정하고, 투자율을 조사하였다. Fe/Co(70$\AA$/15$\AA$)다층막에서 포화자화는 1.8Oe이다. 보자력은 열처리 온도 $250^{\circ}C$까지는 일정한 값(1.8Oe)을 가지나. $250^{\circ}C$ ~ $300^{\circ}C$에서는 약간 증가하고, $300^{\circ}C$이상에서는 갑자기 증가한다. 질소 유량비($N_{2}/Ar+N_{2}$)가 4%인 조건에서 제작한 Fe-N/Co-N 다층박막의 보자력은 5Oe이고, 열처리 온도가 증가함에 따라 감소하다가 $250^{\circ}C$에서 최소값, 2Oe를 나타내고 그 이상의 온도에서 급격히 증가한다.

• 한국재료학회지
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• 제7권1호
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• pp.69-75
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• 1997

$SiO_{2}/CoNiCr/Cr$ 합금 박막을 RF magnetron sputtering 법으로 Cr의 두께를 변화시키면서 제조하였다. 제조된 박막을 진공 열처리하여 열처리 온도에 따른 포화자화, 보자력, 각형비를 조사하였다. $SiO_{2}/CoNiCr/Cr$ 합금 박막에서 포화자화 값은 Cr 하지층의 두께가 증가함에 따라 감소하고 보자력은Cr 하지층의 두께가 증가함에 따라 증가하였다. 이러한 박막의 포화자화 값은 600 emu/cc, 최대 보자력은 550 Oe를 나타내었다. $SiO_{2}/CoNiCr/Cr(1700{\AA})$ 합금 박막에서는 열처리 온도가 증가함에 따라 포화자화 값은 급격히 감소하고 보자력은 증가하였다. 열처리 온도가 $650^{\circ}C$에서 포화자화 값은 as-deposited상태보다도 1/10로 감소하였고 보자력은 1600 Oe로 최대값ㅇ르 나타내었다. Cr 하지층의 두께와 열처리 온도의 증가에 따른 포화자화의 감소는 하지층에서 자성층으로 Cr이 확산하므로써 자기 모멘트의 감소에 의한 것으로 판단된다. 또한 보자력의 증가는 박막 면에 수직한 방향으로 급격한 결정 성장에 기인한 것이다.

• 한국자기학회지
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• 제1권2호
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• pp.55-59
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• 1991

희토류-3d 천이원소인 비정질${[{(Fe_{80}CO_{20})}_{0.98}RE_{0.02}]}_{80}B_{20}(RE=Nd,\;Sm,\;Gd,\;Tb)$ 합금 리본시료에 대한 자기적 성질을 조사하기 위하여 시료진동형 자력계(vibrating sample magnetometor)를 이용하여 77 K부터 900 K까지의 온도 영역에서 포화자화 값을 온도의 함수로 측정 한후, Curie 온도 ($T_{c}$)와 Bloch 상수등을 추정하였다. 이들로 부터 spin wave stiffness 상수, 교환상호작용(exchange interaction)의 범위와 평균자승거리($$)등을 계산하였으며 각 희토류 원소에 대한 치환효과를 비교 분석하였다.

• Journal of Magnetics
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• 제5권4호
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• pp.111-115
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• 2000

Ultrafine $Co_{0.9}Mn_{0.1}Fe_2O_4$ powders have been fabricated by a sol-gel method. Structural and magnetic properties of the powders were investigated by x-ray diffractometry, transmission electron microscopy (TEM), Mossbauer spectroscopy, and vibrating sample magnetometry (VSM). Co-Mn ferrite powders that were fired at and above 773 K contained only a single spinel phase and behaved ferrimagnetically. Powders fired at 673 and 723 K had a spinel structure and were mixed paramagnetic and ferrimagnetic in nature. The magnetic behavior of Co-Mn ferrite powders fired at and above 873 K showed that an increase of the firing temperature yielded a decrease in the coercivity and an increase in the saturation magnetization. The maximum saturation magnetization and coercivity of Co-Mn ferrite powders were 66.7 emu/g and 1523 Oe, respectively, Mossbauer spectra of the powder fired at 923 K were taken at various temperatures ranging from 13 to 850 K. The iron ions.at both A (tetrahedral) and B (octahedral) sites were found to be in ferric high-spin states. The Nel temperature $T_N$ was found to be 850 $\pm$ 2 K. Debye temperatures far A and B sites were found to be $\Theta_A = 757 \pm$5K and $Theta_B = 282 \pm$5 K, respectively.

• 한국자기학회지
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• 제15권2호
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• pp.109-112
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• 2005

Electronic and magnetic properties of $Ti_{1-x}M_xO_{2-\delta}$ (M=Co and Fe) thin films grown by sol-gel method have been investigated. Anatase and rutile $Ti_{1-x}Co_xO_{2-\delta}$ films were successfully grown on $Al_2O_3$ (0001) substrates and exhibited p-type electrical conductivity while the undoped films n-type conductivity. Room temperature vibrating sample magnetometry measurements on the anatase and rutile $Ti_{1-x}Co_xO_{2-\delta}$ films with same x ($=4.8 at.{\%}$) showed quite similar magnetic hysteresis curves with the saturation magnetic moment of $\~4 {\mu}_B$ per Co ion despite their differences in structural and electronic properties. Such giant magnetic moment is attributable to the unquenched orbital moment of the $Co^{2+}$ ions substituting the octahedral $Ti^{4+}$ sites. Similar ferromagnetic behavior was observed for $Ti_{1-x}Fe_xO_{2-\delta}$ films that are highly resistive compared to the Co doped samples. Saturation magnetic moment was found to decrease for higher x, i.e., $\~2$ and $\~1.5 {\mu}_B$ per Fe ion for x=2.4 and 5.8 at. $\%$, respectively. Conversion electron $M\ddot{o}ssbauer$ spectroscopy measurements predicted the coexistence of $Fe^{2+}$ and $Fe^{3+}$ ions at the octahedral sites of $Ti_{1-x}Fe_xO_{2-\delta}$.

• 공업화학
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• 제16권3호
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• pp.372-378
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• 2005

탄산칼슘 포화지수(LI: Langelier Index)는 탄산칼슘의 포화정도로서 수돗물의 부식성을 나타내며 수도관 부식방지를 위해 미국, 유럽, 일본 등은 수도법에 의해 관리되고 있지만 국내는 아직 도입되지 않았다. 본 연구는 LI의 국내 도입 타당성을 검토하기 위해 LI인자(5개항목: 수온, pH, 총알칼리도, 칼슘이온, 전기전도도)들을 측정하고 LI값을 산출하였다. 수온은 연간 $2.0{\sim}26^{\circ}C$, 연평균 $23.9^{\circ}C$로 나타났다. 총알칼리도는 30 mg/L (as $CaCO_3$)로 나타났으며, 총알칼리도를 $HCO_3{^-}$ 농도 값으로 대체가능성을 검토한 결과 농도 차가 거의 없는 것으로 나타났다. LI값은 2.0~-0.5로 나타나 부식성을 가지고 있는 것으로 나타났으며, 수돗물 부식성을 감소시키기 위해 정수장에서 $Ca(OH)_2$, $CaCO_3$, NaOH, $NaHCO_3$ 등을 투입할 필요가 있는 것으로 나타났다.

• 한국전기전자재료학회논문지
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• 제11권6호
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• pp.486-492
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• 1998

The amorphous Co-based magnetic films have a large saturation flux density, a low coercive force, and a zero magnetostriction constant. Therefore, they have been studied for application to magnetic recoding heads and micro magnetic devices. However, it was found that the magnetic anisotropy was changed for each film fabrication processes. In this study, we investigated how to control the anisotropy of sputtered amorphous $Co_{89}Nb{8.5}Zr{2.5}$ films. After deposition, the rotational field annealing ant the uniaxial field annealing were performed under the magnetic field of 1.5 kOe. the annealing was done at the temperature range from 400 to $600^{\circ}C$ for one hour. As-deposited amorphous $Co_{89}Nb{8.5}Zr{2.5}$ thin film had saturation magnetization ($4\piM_5$) of 0.8 T, coercive force($_IH_C$) of 1.5 Oe, and anisotropy field($H_k$) of 11 Oe. The amorphous $Co_{89}Nb{8.5}Zr{2.5}$ thin films annealed by rotational field annealing at $500^{\circ}C$ for one hour was found to be isotropy, and $4\piM_5$ of 0.9 T was obtained from these films, Also, the magnetic anisotropy of as-deposited films could be controlled by uniaxial field annealing at $400^{\circ}C$ for one hour. Anisotropy field($H_k$) of 17 Oe and $4\piM_5$ of 1.0 T were obtained by this method.

• KIEE International Transaction on Electrical Machinery and Energy Conversion Systems
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• 제11B권2호
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• pp.15-21
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• 2001

This paper presents an improved characteristic analysis methodology for a 5-phase hybrid stepping motor. The basic approach is based on the use of equivalent magnetic circuit taking into account the localized saturation throughout the hybrid stepping motor. The finite element method(FEM) is used to generate the magnetic circuit parameters for the complex stator and rotor teeth and airgap considering the saturation effects in tooth and poles. In addition, the neural network is used to map a change of parameters and predicts their approximation. Therefore, the proposed method efficiently improves the accuracy of analysis by using the parameter characterizing localized saturation effects and reduces the computational time by using the neural network. An improved circuit model of 5-phase hybrid stepping motor is presented and its application is provided to demonstrate the effectiveness of the proposed method.

• Journal of Advanced Marine Engineering and Technology
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• 제29권3호
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• pp.297-305
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• 2005

The evaporation heat transfer coefficient of $CO_2$ (R-744) in a horizontal tube was investigated experimentally. The experiments were conducted without oil in a closed refrigerant loop which was driven by a magnetic gear pump. The main components of the refrigerant loop are a receiver. a variable-speed pump. a mass flow meter. a pre-heater and evaporator (test section). The test section consists of a smooth. horizontal stainless steel tube of 7.75 mm inner diameter. The experiments were conducted at mass flux of 200 to $500\;kg/m^{2}s$. saturation temperature of $-5^{\circ}C\;to\;5^{\circ}C$. and heat flux of 10 to $40\;kW/m^2$. The test results showed the evaporation heat transfer of $CO_2$ has greatly effect on more nucleate boiling than convective boiling. The evaporation heat transfer coefficients of $CO_2$ are highly dependent on the vapor quality. heat flux and saturation temperature. The evaporation heat transfer coefficient of $CO_2$ is very larger than that of R-22 and R-134a. In making a comparison between test results and existing correlations. the present experimental data are the best fit for the correlation of Jung et al. But it was failed to predict the evaporation heat transfer coefficient of $CO_2$ using by the existing correlation. Therefore. it is necessary to develop reliable and accurate predictions determining the evaporation heat transfer coefficient of $CO_2$ in a horizontal tube.