• Journal of the Korean Society for Aeronautical & Space Sciences
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• v.45 no.2
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• pp.106-113
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• 2017

Attitude determination algorithms for aircraft and land vehicles use earth gravitational vector and geomagnetic vector; hence, magnetometers and accelerometers are employed. In dynamic situation, the output from accelerometers includes not only gravitational vector but also motional acceleration, thus it is hard to determine accurate attitude. The acceleration compensation method treated in this paper solves the problem to compensate the specific force vector for motional acceleration calculated by a GPS receiver. This paper analyzed the error from the corrected vector regarded as a constant by conventional acceleration compensation method, and improve the error by rederivation from measurements. The analyzed error factors and improvements by the proposed algorithm are verified by computer simulations.

• Progress in Superconductivity
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• v.8 no.2
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• pp.164-168
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• 2007

We developed a SQUID magnetometer based on Double Relaxation Oscillation SQUID(DROS) for measuring magnetocardiography(MCG). Since DROS provides a 10 times larger flux-to-voltage transfer coefficient than the conventional DC-SQUID, simple flux-locked loop electronics could be used for SQUID operation. Especially, we adopted an external feedback to eliminate the magnetic coupling with adjacent channels. When the DROS magnetometer was operated inside a magnetically shielded room, average magnetic field noise was about 5 $fT/^{\surd}Hz$ at 100 Hz. Using the DROS magnetometer, we constructed a multichannel MCG system. The system consisted of 61 magnetometers are arranged in a hexagonal structure and measures a vertical magnetic-field component to the chest surface. The distance between adjacent channels is 26 mm and the magnetometers cover a circular area with a diameter of 208 mm. We recorded the MCG signals with this system and confirmed the magnetic field distribution and the myocardinal current distribution.

• Journal of the Korean Magnetics Society
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• v.7 no.1
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• pp.7-12
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• 1997

Amorphous $Fe_{50}Zr_{50}$ alloy has been manufactured by mechanical alloying from pure elemental powders of Fe and Zr in conventional ball mill under an Ar atmosphere. Structure and magnetic properties of the amorphous phase were studied by transmission electron microscopy and SQUID magnetometry. Selected area diffraction patterns taken from the mechanically alloyed powders showed two halo rings, indicating coexistence of Fe rich and Zr rich amorphous phases in mechanically alloyed powder. Curie temperature of the Fe rich amorphous phase, measured by Arrot plot, was 195 K. Fe content in the ferromagnetic amorphous phase, estimated from the Curie temperature, was about 65 at%. Spin wave stiffness constant of $Fe_{50} Zr_{50}$ alloys processed for 100 and 200 hrs were 52.2 and 63.8 meV, respectively. The higher spin wave stiffness constant in 200 hrs milled powders may arise from the precipitation of $\alpha$-Fe by partial crystallization of amorphous phase.

• Journal of the Korean Magnetics Society
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• v.16 no.5
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• pp.249-254
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• 2006

CoFeNi alloys are some of the most studied soft magnetic materials because of their superial properties over FeNi alloys as write head core materials in HDD and MEMS. We studied the effect of magnetic property according to size and orientation of crystal for electroplated Co-Fe-Ni alleys. In case of heat treated ternary alloy, it affect the change of crystal size and structure. In this study, it intends to improve the magnetic properties of CoFeNi thin film by heat treatment. Minimized coercivity and increased magnetization are due to heat treatment from $300^{\circ}C\;to\;400^{\circ}C$. As a bcc phase formation, it grow to amount of magnetization.

• Journal of the Korean Crystal Growth and Crystal Technology
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• v.28 no.1
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• pp.21-27
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• 2018

Synthesis of ferromagnetic composite materials for the $Cu-BaFe_{12}O_{19}$ system by mechanical alloying (MA) has been investigated at room temperature. A mixture of copper and barium ferrite with a weight ratio of $Cu:BaFe_{12}O_{19}=4:1$, 3 : 2, 2 : 3 and 1 : 4 was used. It is found that $Cu-BaFe_{12}O_{19}$ composite powders in which $BaFe_{12}O_{19}$ is dispersed in copper matrix are successfully produced by mechanical alloying of $BaFe_{12}O_{19}$ with Cu for 80 min. in all composition. The change in X-ray diffraction patterns and magnetic properties reflects the details for the formation of ferromagnetic metal matrix composite of pure Cu and $BaFe_{12}O_{19}$ during mechanical alloying. Magnetization of $Cu-BaFe_{12}O_{19}$ composite powders gradually increases with increasing the amounts of barium ferrite, whereas coercive force of MA powders gradually decreases due to the refinement of barium ferrite powders with ball milling. However, it can be seen that the coercivity of $Cu-BaFe_{12}O_{19}$ MA composite powders with a weight ratio of $Cu:BaFe_{12}O_{19}=4:1$ and 3 : 2 ball-milled for 80 min. is still high value of 1400 Oe and 1450 Oe, respectively suggesting that the refinement of barium ferrite powders during ball milling process tend to be suppressed due to the ductile copper.

• Journal of the Korean Magnetics Society
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• v.10 no.5
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• pp.225-231
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• 2000

The crystallographic and magnetic properties of the sample F $e_{0.8}$ $Co_{0.18}$(BN)$_{0.02}$ synthesized by microwave arc-melting with the maximum power of 3.5 kW have been studied by the methods of an X-ray diffraction and the measurement of the magnetic hysteresis using the vibrating sample magnetometer at room temperature. The samples were prepared in a form of pellet pressed under the pressure of 9,000 N/c $m^2$, rolled coldly, and treated with the different temperatures. The X-ray diffraction pattern of pelleted sample shows that the crystal structure of the sample is bcc as same as that of Fe with a good uniformity. The X-ray diffraction pattern shows that a residual stress, which exists in the sample, is eliminated by final 90$0^{\circ}C$ annealing. As rolling rate and heat treatment temperature increases, the saturation magnetization and the remanence of the samples increase whereas the coercivity of the samples shows decrease. Also the saturation magnetization and the remanence of the samples were affected by rolling rate and rolling direction than heat treatment temperature, but the coercivity of the samples was affected by rolling rate and direction as well as heat treatment temperature. This means that a domain wall motion is easy due to elimination of a residual stress and an inclusion which exists in the sample by rolling and heat treatment and a local induced-magnetization easy axis was also formed to parallel to the rolling direction due to creation of the like-atom pairs across the slip plane by rolling......

• Korean Journal of Materials Research
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• v.7 no.2
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• pp.136-139
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• 1997

증착법을 이용하여 $Sm(Co_{1-x}Fe_{x})$ 및 $Sm_{2}(Co_{1-x}Fe_{x})_{17}$(X=0, 0.3,0.5,0.7)박막을 제작하여 조성변화 및 열처리 온도 변화에 따른 자기적 성질의 변화에 대해 검토 하였다. Fe의 양이 증가 할 수록 포화자화 값은 증가 하지만 각형비는 감소하였고 보자력도 약간 감소하는 경향을 보였다. $Sm(Co_{0.5}Fe_{0.5})_{5}$ 조성박막의 경우, $800^{\circ}C$, 20분 열처리에 의해 약 6.1MGOe의 $(BH)_{max}$을 보였다. 본 박막자석의 자기적 성질의 증대를 위해서는 시료제작 방법의 개선이 필요하다고 사료 된다.

• Bulletin of the Society of Naval Architects of Korea
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• v.30 no.2
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• pp.8-10
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• 1993

선박에너지 개발을 위한 미래의 유력한 추진체로서 초전도 자력장을 이용한 선박을 들 수 있는데 이와 같은 경우에는 실험을 하기에는 비용이 엄청나게 소요되고 설비 자체가 복잡하기 때문에 CFD를 이용해서 초기 계\ulcorner을 구상하고 선체 주위의 유동장의 제어 및 기초 설계를 하여야 할 것이다. CFD계산을 통해 일반적으로 얻을 수 있는 것은 -압력 분포 -자유 표면 파고 -유속 분포 -유선 추적 -선체 표면의 응력 분포 -한계 유선 분포 -선미 와류 생성 과정 -선체 저항 계산 등으로 선형 개발에 필요한 기본 자료들이다. 여기서 CFD의 유용가치를 강조할 수 있는데 위의 많은 데이터를 실험을 통해서 얻으려면 막대한 경비와 노력이 투입되어야 한다. 또한 현재의 실험 시설로는 정량적으로 측정할 수 없는 부분도 일부 있다. CFD의 경우는 그러한 어려움은 없으나 꼭 필요한 것이 수치계산의 검증이다. 계산 결과의 유효성(validity)을 검증해야 한다는 의미이다. 계산은 실험을 통하여 반드시 비교 검토가 이루어져야 하며 이의 수단으로 선박 분 야에서는 Wigley 모형이나 Series 60와 같은 것들이 사용되고 잇다. 당 연구소의 저항추진연구 실에서는 CFD의 연구가 수년 전부터 소수의 인원을 중심으로 이루어져 왔다. 이와 관련하여 대표적인 몇 가지만 소개하고자 한다.

• Journal of the Korean Magnetics Society
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• v.2 no.1
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• pp.56-60
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• 1992

광자기 디스크의 자기 및 기록특성에 SiN 하지층이 미치는 영향에 대해서 연구하였다. PC기관에 4층구조막의 디스크를 DC 마그네트론 스퍼터링에 의해 성막하였으며 스퍼터링 압력이 증가함에 따라 SiN 박막의 표면이 거칠어 지고 주상형성장이 현저하게 나타났다. SiN 하지층의 비세조직의 변화는 자기기록막의 보자력, 수직이방성 등에는 영향을 미치지 않았지만 지구의 형 성과정은 SiN 하지층의 조직에 따라 민감하게 변화하였다. SiN 하지층이 Porous 할수록 광자기 디스크의 기록이 이루어 지는 임계파우워 값이 작고, 또한 자구의 형성이 이루어 지는 임계외자 계의 크기도 넓은 범위에서 나타났다. 광자기 디스크의 기록특성을 증대시키기 위해서는 자기기 록막의 성능과는 관계없이 치밀하고 표면이 평할한 SiN 하지층을 증착하는 것이 필수적임을 관 찰하였다.

• Journal of the Korea Academia-Industrial cooperation Society
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• v.5 no.5
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• pp.395-402
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• 2004

We need to develop technology of identifying high temperature high pressure(HTHP) synthetic diamond and HTHP treated natural diamonds from untreated natural diamonds to cope with sophisticated diamond enhancing technology. We had successfully identified synthetic diamonds using a vibrating sample magnetometer due to their ferromagnetic property. In addition, we identified the HTHP enhanced TypeIa, TypeIIa diamonds by employing non-destructive Fourier Transform Infrared(FTIR) spectroscopy.