• Journal of Magnetics
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• 제2권2호
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• pp.55-57
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• 1997

A mutual-inductance bridge type ac magnetic susceptibility measurement system was built in our laboratory. With addition of a phase-sensitive prestage, it was simple to implement and provided a high signal-to-noise (S/N) ratio.

• 한국자기학회지
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• 제26권1호
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• pp.13-18
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• 2016

유기 용매에 고르게 분산되어 있는 26 nm 크기의 산화철 나노입자를 사용하여 주파수에 따른 교류 자화율을 측정하였다. 자기장이 없는 조건에서 측정한 나노입자의 자화율은 Debye 완화 모델로 계산한 결과와 일치하였으며, 완화 주파수(relaxation frequency)는 370 Hz였다. 나노입자의 완화 주파수는 용매의 점성에 의한 브라운 운동(Brownian motion)의 완화 시간과 일치하였다. 브라운 운동에 의한 나노입자의 완화 주파수는 자기장의 세기에 따라 선형적으로 증가하는 특성을 보였다.

• Journal of Magnetics
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• 제11권4호
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• pp.189-194
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• 2006

The recent development of bio-conjugated magnetic nanoparticles offers many opportunities for applications in the field of biomedicine. In particular, the use of magnetic nanoparticles for biosensing has generated widespread research efforts following the progress of various magnetic field sensors. Here we demonstrate substrate-free biosensing approaches based on the Brownian rotation of ferromagnetic nanoparticles suspended in liquids. The signal transduction is through the measurement of the magnetic ac susceptibility as a function of frequency, whose peak position changes due to the modification of the hydrodynamic radius of bio-conjugated magnetic nanoparticles upon binding to target bio-molecules. The advantage of this approach includes its relative simplicity and integrity compared to methods that use substrate-based stray-field detectors.

• Journal of Magnetics
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• 제16권4호
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• pp.368-373
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• 2011

Particle size distributions in 10 nm magnetite ferrofluids are analyzed based on both dc and ac magnetic measurements. Modified log-normal distributions are used for fitting the experimental results, which allows for a proper account of the narrow distributions. The calculated average particle sizes are in good agreement with the TEM results. However the ac method gives a much narrower distribution width than that of the dc magnetization curve fit. The proposed measurements combined with the analysis methods are useful for the characterization of ferrofluids being considered for biomedical applications.

• 한국자기학회지
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• 제5권3호
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• pp.179-184
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• 1995

{100} 철단결정에 자기장을 가해주거나 혹은 자기장 없이 전류만을 변화 시킬 때의 교류 자기감수율에 관하여 연구 하였다. 작은 자기장과 전류를 철단결정에 걸어줄때, 단결정의 단연적 중앙끈처에는 정사각형 자구가 형성된다. 실험을 통하여 이 자구의 자기화 방향으로 자장을 걸어주변 걸어주는 전류크기와 전류방향의 영향을 받음을 보인다. 이 실험 결과는 전류에의해 중앙에 형성된 자구가 전류의 증감함에따라 변화하는 자구크기로 설명할 수 있다. 실험으로 측정된 자기강수율을 설명하기 위하여 미세 자기이론을 사용하였으며, energy 값을 구히기 위하여 간단한 model을 설정하였다. 이 model로부터 교류 자기감수율을 구할 수 있었으며, 이때 계산한 교류 자기감수율은 한 안정된 구조에서 다른 안정된 구조로 변화하는 전류를 제외한 거의 대부분 전류에 대하여 정량적으로 설명할 수 있었다.

• Transactions on Electrical and Electronic Materials
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• 제9권6호
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• pp.265-272
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• 2008

In this paper, AC losses of long wire Bi-2223 tapes with different twist pitch of superconducting core were fabricated, measured and analyzed. These samples produced by a powder-in-tube method are multi-filamentary tape with Ag matrix. Also, it's produced by non-twist. The critical current measurement was carried out under the environment in Liquid nitrogen and in zero field by 4-prob method. And the Magnetic measurement was carried out under the environment of applied time-varying transport current by transport method. From experiment, the susceptibility measurements were conducted while cooling in a magnetic field. Flux loss measurements were conducted as a function of ramping rate, frequency and field direction. The AC flux loss increases as the twist-pitch of the tapes decreased, in agreement with the Norris Equation. Neutron-diffraction measurements have been carried out investigate the crystal structure, magnetic structures, and magnetic phase transitions in Bi-2223([Bi, Pb]:Sr:Ca:Cu:O).

• KIEE International Transactions on Electrophysics and Applications
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• 제5C권5호
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• pp.204-210
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• 2005

Alternating current (AC) losses of two Bi-2223 ([Bi, Pb]: Sr: Ca: Cu: O = 2:2:2:3) tapes [(Tape I, un-twist-pitch) and the other with a twist-pitch of 10 mm (Tape II)] were measured and compared. These samples, produced by the powder-in-(Ag) tube (PIT) method, are multi-filamentary. Also, it's produced by non-twist and different twist pitch (8, 10, 13, 30, 50 and 70 mm). The critical current measurement was carried out under the environment in liquid Nitrogen and in zero-field by 4-probe method. Susceptibility measurements were conducted while cooling in a magnetic field. Flux loss measurements were conducted as a function of ramping rate, frequency and field direction. The AC flux loss increases as the twist-pitch of the tapes decreased, in agreement with the Norris Equation. Neutron-diffraction measurements have been carried out investigate the crystal structure, magnetic structures, and magnetic phase transitions in Bi-2223([Bi, Pb]:Sr:Ca:Cu:O)

• 한국자기학회지
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• 제5권5호
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• pp.815-818
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• 1995

Ac susceptibility of iron-nitride magnetic fluids with various particle number densities was measured. Therelaxation time increases rapidly as the temperature decreases or the inter-particle interaction increases. The analysis of the data suggests that the activation energy is proportional to ${(k_{B}T/J_{typ})}^{\alpha}$ with $\alpha$~-0.24 in the lower temperature range in which the thermal energy is comparable to the magnetic dipole interaction.

• Progress in Superconductivity
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• 제7권1호
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• pp.22-27
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• 2005

We have studied the standardization of critical temperature measurements by using an ac susceptometer. Wire forms of NbTi, $Nb_{3}Sn$, and Bi-2223 superconductors were prepared to measure the temperature dependences of the magnetization. In order to study the optimum ac magnetic field and frequency, various amplitudes from 2 Oe to 10 Oe with frequencies from 11.3 Hz to 1033 Hz were applied to three specimens. Analytical comparison of the magnetic curves with the resistive curves was accomplished to investigate validity of using the new method.

• 한국자기학회지
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• 제5권5호
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• pp.372-375
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• 1995

The magnetization pattern of the central cross section deduced from the ac susceptibility measurement is described with an analytical function. The function is based on a charge-free configuration. The thickness of the $^{\circ}$ wall lying in a (100) plane and the wall energy are calculated analytically. Total energy of the domain structure has been minimized with Ritz's method. As the result of the minimization, the energy density of the $^{\circ}$ wall lying in a (100) plane is $0.58\;erg/cm^{2}$ and the one for a (110) plane is $1.18\;erg/cm^{2}$. Thicknesses of these walls are calculated numerically. Also, the calculation indicates there is a small central domain at the cross section without applied current. With the ac susceptibility measurement the existence of the domain without current can be identified.