• Journal of the Korean Magnetics Society
• /
• v.3 no.2
• /
• pp.135-138
• /
• 1993

Saturation rnagnetostriction and rnagnetoelastic properties of amorphous $Fe_{82}B_{18-x}Al_{x}$ and $Fe_{80}B_{20-x}Al_{x}$ alloys have been studied. Saturation magnetostriction of the alloys has increased according to the increase of AI content. The amorphous $Fe_{82}B_{14}Al_{4}$ alloy shows the highest saturation magnetostriction of 45 ppm among the alloy systems. The ratio of maximum magnetic induction change to tensile stress of this alloy is about $0.026\;T.mm^{2}/N$, and it is considered to be applicable for a high resolution mechanical sensor.

• Journal of the Korean Magnetics Society
• /
• v.8 no.3
• /
• pp.125-130
• /
• 1998

13Cr-1.5Nb-Fe alloy powder was fabricated by water atomization method, and ring-shape specimen of this composition was fabricated by oil press, and then sintered in the vacuum furnace. Powder shape, size distribution, composition (C, N, O, S) analysis and saturation magnetization of as-prepared 13Cr-1.5Nb-Fe alloy powder were investigated. Ac permeability and power loss was measured after forming and sintering process. Saturation magnetization and contents of oxygen of the alloy powder is160 emu/g and about 6000 ppm, respectively. 50 % volume fraction indicate particle size of 70$\mu$m. The ac permeability of sintered specimen increases with increasing sintering temperature and forming pressure. The power loss is 107 W/cc at sintering temperature of 1200 $^{\circ}C$, 12 ton/$\textrm{cm}^2$ forming pressure, and 20 KHz. It is the lowest among the prepared specimen.

• Transactions of the Korean Society of Mechanical Engineers A
• /
• v.34 no.7
• /
• pp.821-827
• /
• 2010

This paper proposes a density method based topology optimization of a perpendicular magnetic recording system design in which the saturation effect is taken into account. During the topology optimization process in magnetic fields, the magnetic reluctivity is updated in accordance with the changes in element density determined by a sensitivity analysis. The magnetic reluctivity is determined from a B-H curve and is used to represent nonlinear material property, i.e., the saturation effect. The sensitivity for a generalized response functional is formulated using the adjoint variable method in which the nonlinear property is taken into account and the objective function is set such that the magnetic energy in the media is maximized. Effects due to the nonlinear property can be observed from a numerical study in which the linear and the nonlinear topology optimization results are compared.

• Journal of the Korean Magnetics Society
• /
• v.3 no.4
• /
• pp.289-292
• /
• 1993

[Ni/Fe/Cu] and [Fe/Ni/Fe/Cu] multilayers were prepared with three gun rf-magnetron sputtering, and dependence of magnetoresistance on the Ni IFe thickness ratio was investigated. Vaccum annealing was tried to invetigated the effect of annealing. Oscillation of magnetoresistance on the Cu spacer thickness was dbserved in these two kinds of multilayers. When the thickness of Fe inserted into the Ni/Cu interface was about $3\;\AA$. the maximum value of magnetoresistance(13 %) could be observed. In a sample of $1~2\;\AA$ Fe thickness, saturation field decreased significantly, while magnetoresistace decreased slightly in comparison with the sample of $3\;\AA$ Fe. In ${[Cu(23\;\AA)/Fe(1\;\AA)/Ni(18\;\AA)/Fe(1\;\AA)]}_{20}/Fe(80\;\AA)/Si$, 6 % magnetoresistance with 100 Oe saturation field could be obtained. No appreciable change in magnetoresistance and saturation field could be observed by low temperature annealing. Formation of Ni-Fe alloy was not confinred.

• The Journal of the Korea institute of electronic communication sciences
• /
• v.10 no.7
• /
• pp.781-786
• /
• 2015

In this paper, we analyzed characteristic of window type current transformer and we performed the optimal design consider to the loss; in order to design the current transformer figured signal of overcurrent warning circuit. The core size of window type current transformer was determined by the secondary coil turns. We analyzed current waveform, which is appeared by the number of coil turns on the core, we made sure the relation of secondary coil turns and load resistance in order to improve the non-sinusoidal wave by the flux saturation of the current transformer core. Additionally, we did improvement of the accuracy and optimal design through the transformation of the inner diameter and the stack length when the outer diameter of core is sustaining.

• Proceedings of the Korea Crystallographic Association Conference
• /
• 2003.05a
• /
• pp.9-9
• /
• 2003

최근에 Fe-CU, Fe-Si 등과 같이 자성금속과 비자성금속화합물에 대한 연구가 활발히 진행되고 있다. 본 연구에서는 기계적 합금법으로 제작한 Co/sub 5/C/sub 95/ 나노미립상 합금의 구조와 자기적 성질을 조사하였다. 그림(1)은 EXAFS 스펙트럼의 푸리에변환이다. 이로부터 합금화시간에 따라 Co-Co 결합은 점차적으로 작아지며 Co-C 결합이 진행됨에 알수 있다. 그림(2)은 합금화시간에 따른 포화자화값과 보자력의 크기이다. 포화자화는 합금화 시간에 따라 연속적으로 작아졌으며 보자력은 커지다가 작아지는 경향을 보였다. 포화자화가 작아지는 것은 Co-C 결합이 생기면서 Co의 쌍을 이루지 않은 전자가 C의 전자와 쌍을 이루면서 상쇄되기 때문인 것으로 보인다. 보자력의 거동은 Co 미립자가 다자구영역으로부터 단자구영역으로 전환되기 때문인 것으로 해석될수 있다. Co 미립자는 C의 캡슐형에 싸여있으며 60시간과 100시간에서 Co 미립자의 크기는 X-ray 회절선의 넓어짐으로부터 Scherrerr 공식을 이용하여 계산한 결과 18nm 와 15nm 정도가 됨을 알 수 있었다. 연구를 통하여 Co/sub 5/C/sub 95/ 나노미립상합금을 기계적합금법으로 만들 수 있음을 알 수 있었다. 이론적인 계산에 의하면 초상자성 Co 입자의 크기는 8.2nm 정도가 되었으며 본 실험에서 최종 입자의 크기는 15nm까지 작아졌다.

• Journal of the Korean Magnetics Society
• /
• v.8 no.4
• /
• pp.231-240
• /
• 1998

We investigated that the fabrication and reproducing signal characteristics of tri-layered magnetoresistance (MR) element for the high density magnetic thin film heads and sensors. Magnetoresistance curve of tri-layered MR element predicted by computer modeling was saturated above external field of -15 Oe~+22 Oe, and it was shifted to linearized region as large as 4 Oe. In the case of fabricated real device, magnetoresistance curve was saturated above external field of $\pm$15 Oe, and it was shifted to linearized region as large as 4 Oe. As shown in real device, MR response curve was in good agreement with the simulation results. As a result of experimental data of reproducing output signal in real device, it retained normal sinusoidal waveforms in 1~4 Oe external magnetic field. In this magnetic field region, the fabricated heads with tri-layered MR element can be operated with good reproduced characteristics. This will be beneficial to the use of efficient processes of manufacturing elements and the vacuum deposition techniques which control thin film properties.

• 전기의세계
• /
• v.12
• /
• pp.30-34
• /
• 1963

비선형자기철심을 사용한 inductance를 그 비선형영역까지 동작하게 할때와 직렬형가포화 reactor에 R-C부하를 직렬로 연결하여 동작시킬 때 어떠한 동작범위에서는 회로의 전류진폭이 불안정한 경우가 있다. 특히 직렬형가포화 reactor에 R-C부하를 연결한 경우는 J.T.Salihi씨 및 H.C.Bourne씨에 의하여 그 동작현상이 설명되었다. 그러나 안정조건은 충분한것이 아니라고 생각되며 이와같은 R-L-C 직렬회로는 정량적으로 해석하는데 수학적인 난점이 있어서 곤란하지만 정성적인 방법 즉 근사계산에 의하여 안정성문제와 그 회로동작상태 등을 고찰할 수 있다. 본 고는 이러한 안정조건을 계산하여 제시코져 한다.

• Proceedings of the KSMRM Conference
• /
• 2002.11a
• /
• pp.95-95
• /
• 2002

목적： 기존의 척추용 코일은 phased array 코일을 주로 많이 사용하여 왔다. Phased array 코일은 여러개의 표면 코일로 구성되어 있어 RE 자기장의 영역이 표면코일과 비슷하다. 그래서, 척추 영상을 얻기 위해서는 다른 부위의 핵 스핀을 포화시키는 불편함이 있다. 기존의 표면 코일보다 RF penetration depth가 적은 theta coil을 이용하여, 척추에 적합한 코일을 개발했다. 대상 및 방법： theta coil을 길게 제작하여 척추에 적합하게 하였다. 코일의 길이는 약 35cm, 폭은 16cm이다. 수신 전용으로 하기 위해서, 다이오드를 이용하여 detune 회로를 포함하였다. 기존의 코일과 비교하기 위해 theta coil과 GE사의 척추용 코일로부터 각각 영상을 획득하였다.

• Journal of Sensor Science and Technology
• /
• v.1 no.1
• /
• pp.23-34
• /
• 1992

In order to fabricate magnetoresistive sensor, Fe-Ni and Co-Ni alleys were evaporated on the slide glass and the silicon wafers. Saturation magnetic induction($B_{s}$), coercive field strength($H_{c}$) and magnetoresistance were measured for fabricated samples. The evaporated Fe-Ni thin films show that the saturation magnetic induction was 0.65 T, and coercive field strength was 0.379 A/cm, and this value was changed to 0.370 A/cm(//), 0.390 A/cm(${\bot}$), respectively after magnetic annealing. For the measurement of coercive field strength, magnetizing frequency of 1 kHz was used. For the fabricated sensor element, the change of magnetoresistance (${\Delta}R/R$) was excessively unstable due to oxidation in the process of fabrication. The evaporated Co-Ni alloy thin films show that saturation magnetic induction was 0.66 T, and coercive field strengthes were 5.895 A/cm(//), 5.898 A/cm(${\bot}$), respectively, after magnetic annelaing. The change of magnetoresistance(${\Delta}R/R$) was $3.6{\sim}3.7%$ of which value was excessively stable to room temperature. Fe-Ni thin film could have many problems due to large affinity in the process of fabrication of magnetoresistance sensor, but Co-Ni thin film could be a suitable material for fabrication of magnetoresistance sensor, because of its small affinity and definite magnetoresistance effects.