• 방사성폐기물학회지
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• 제3권2호
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• pp.113-123
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• 2005

자기필터시스템을 이용한 원자로 냉각재로부터의 방사성 부식생성물 제거는 원자력 발전소의 운전 및 유지보수 종사자에 대한 방사선 피폭 준위를 낮추는 방법으로 많은 연구가 이루어지는 분야 중 하나이다. 그 결과, 보다 높은 신뢰성과 여과성능을 갖춘 자기필터를 개발하고자 수화학 분야에서는 많은 연구가 이루어지고 있다. 본 연구에서는 부식생성물의 자기적 성질을 이용하여 원자력 발전소 냉각재내의 방사성 부식생성물을 제거하기 위해 영구자석과 전자석 이 조합된 자기필터 시스템을 개발하였다. 영구자석은 부식생성물의 여과를 위해 사용되며 전자석은 아주 미세한 콜로이드 부식생성물 입자의 크기를 증가시키기 위한 응집에 이용된다. 선행 연구에서 영구자석만을 사용한 필터 실험결과 대부분의 부식생성물 입자에 대해 만족할만한 수준의 제거효율을 달성하였으며 특히, 크기가 5$\mu$m 이상인 입자의 경우 제거효율은 90$\%$를 상회하였다. 전자석을 이용한 응집 실험결과 화학응집제의 첨가 없이 대부분의 부식생성물 입자가 전자기장에 의해 응집하여 크기가 5$\mu$m 이상으로 증가되어 응집실험에 대해 전반적으로 만족스러운 결과를 도출하였다. 따라서, 영구자석과 전자석이 조합된 자기필터시스템은 방사성 부식생성물 제거를 위한효과적인 방법으로 높은 제거효율을 보여주리라 여겨진다.

• 한국자기학회지
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• 제22권6호
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• pp.221-227
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• 2012

고특성 영구자석은 하이브리드 및 전기자동차의 구동모터와 풍력발전에 적용되면서 크게 주목을 받고 있다. Nd-Fe-B 영구자석은 가장 높은 최대자기에너지적을 가지고 있지만 고온(${\sim}200^{\circ}C$)의 구동환경에서는 보자력이 급격히 감소하기 때문에 사용할 수 없는 단점을 가지고 있다. 그러므로 큰 보자력을 가지는 Nd-Fe-B 영구자석에 대한 개발이 요구되고 있다. Nd-Fe-B 소결자석에서 보자력을 증가시키기 위해서는 Nd를 Dy 또는 Tb으로 치환하면 쉽게 증가시킬 수 있다. 그러나 이들 원소는 Fe와 반강자성 결합을 하여 잔류자속밀도를 낮추고, 적은 매장량과 한정된 지역에 편재되어 있어 수요급증에 따른 자원수급 및 가격 급등의 문제를 가지고 있다. 따라서, Dy 및 Tb과 같은 중희토류를 사용하지 않거나 최소한의 양을 사용하여 보자력을 증가시키고자 하는 연구가 많이 진행되고 있다. 본 논문에서는 이러한 중희토류 원소의 저감 및 대체에 대한 연구들을 소개하고자 한다.

• Progress in Superconductivity
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• 제12권2호
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• pp.93-98
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• 2011

Pinning force is the mechanism between a superconductor and a permanent magnet and it provides a stable levitation. However, when external force greater than the pinning force such as the earthquake exerts, the levitated object may lose the levitating characteristic. In order to achieve more stabilized levitation, the copper plate was inserted in between a superconductor and permanent magnets. And by applying the eddy current effect caused from the relationship between a copper plate and permanent magnets, more stabilized levitation can be established. In this study, an optimized design was found based on various configurations of permanent magnet's polarity, thickness and area of copper plate, and the gap distance between copper plate and permanent magnet. As results, higher eddy current value was obtained at where the change of polarity exists in permanent magnet configuration, and the highest eddy current value was observed at the copper plate thickness of 5 mm and the area of 80 mm ${\times}$ 80 mm. From the resulted optimized conditions above, which are 7 mm gap distance between a superconductor and permanent magnets and 80 mm ${\times}$ 80 mm ${\times}$ 5 mm dimension of a copper plate, the stiffness value was 65 % increased comparing to without any copper plate insertion.

• 한국정밀공학회지
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• 제19권7호
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• pp.125-132
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• 2002

This paper shows an experimental magnetic levitation table using one degree-of-freedom active control. The magnetic levitation table using repulsions of permanent magnets was theoretically presented already. Thus the objective of this paper is to prove stable levitation with only one degree-of-freedom active control experimentally. For the design of the system, at first, permanent magnets are selected. Secondly, the spring constants of the virtual spring are obtained by simulation. Thirdly, the moving magnets are arranged using a stable layout relation. Fourthly, a linear voice coil motor is designed. Finally, the magnetic levitation system is manufactured. The phenomenon of stable levitation in the manufactured table is proven by means of dynamic time and frequency responses. The differences between the theoretical natural frequencies and experimental ones are analyzed. Also, stable range in the control direction is shown experimentally.

• 전기학회논문지
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• 제64권12호
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• pp.1703-1708
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• 2015

This paper deals with the position and torque control of a toroidal type rotor which has a magnetic bearing structure. The proposed magnetic bearing structure supports the rotor by the repulsive forces of permanent magnets, and has a two degree of freedom for rotor position when the rotor is rotating. Permanent magnets and coils in the stator allow for a two degree of freedom control of the rotor position and torque generation by reacting with permanent magnets of the rotor. The executed gyro actuator has a number of poles such as five-phase permanent magnet motors and 10 stator coils for the rotor position control. In this study, the verification of the stability of the magnetic bearing was conducted using the equation of motion when the rotor was rotating, and the coil current commutation method for the position control and torque generation was studied. As a result, the feasibility of the proposed structure and control was verified by simulations of Finite Element Method (FEM) and experiments using the executed gyro actuator.

• Journal of Magnetics
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• 제7권2호
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• pp.55-58
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• 2002

MR transfer behaviors of the permanent magnet biased spin valve MR sensors with SyAF (synthetic antiferromagnet) layers were studied by micromagnetics modeling. For narrow track MR heads, various height to width ratios were considered together with strength of permanent magnets which stabilities the free layed As the MR sensor width is reduced to $0.12 \mu{m}$, sensor height less than 0.09 ${\mu}{\textrm}{m}$ is needed to show good linearity and the Mr.t of permanent magnets smaller than 0.2 memu/$cm^2$ is sufficient for the domain stabilization. The conditions for single domain behavior of the free layer were also investigated through optimizing the biasing strength of permanent magneto the shield gap and the aspect ratio of MR sensor.

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2015년도 자성 및 자성재료 국제학술대회
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• pp.175-175
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• 2015

• 한국자기학회:학술대회 개요집
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• 한국자기학회 2008년도 Asian Magnetics Conference
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• pp.93.1-93.1
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• 2008

• 전기저널
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• 4호통권112호
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• pp.30-35
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• 1986

• 한국분말재료학회지
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• 제26권2호
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• pp.146-155
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• 2019

Rare earth magnets are the strongest type of permanent magnets and are integral to the high tech industry, particularly in clean energies, such as electric vehicle motors and wind turbine generators. However, the cost of rare earth materials and the imbalance in supply and demand still remain big problems to solve for permanent magnet related industries. Thus, a magnet with abundant elements and moderate magnetic performance is required to replace rare-earth magnets. Recently, $a^{{\prime}{\prime}}-Fe_{16}N_2$ has attracted considerable attention as a promising candidate for next-generation non-rare-earth permanent magnets due to its gigantic magnetization (3.23 T). Also, metastable $a^{{\prime}{\prime}}-Fe_{16}N_2$ exhibits high tetragonality (c/a = 1.1) by interstitial introduction of N atoms, leading to a high magnetocrystalline anisotropy constant ($K_1=1.0MJ/m^3$). In addition, Fe has a large amount of reserves on the Earth compared to other magnetic materials, leading to low cost of raw materials and manufacturing for industrial production. In this paper, we review the synthetic methods of metastable $a^{{\prime}{\prime}}-Fe_{16}N_2$ with film, powder and bulk form and discuss the approaches to enhance magnetocrystalline anisotropy of $a^{{\prime}{\prime}}-Fe_{16}N_2$. Future research prospects are also offered with patent trends observed thus far.