• Bulletin of the Korean Space Science Society
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• 2003.10a
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• pp.83-83
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• 2003

자기 폭풍 발생시에 지구 자기권 내에서 MeV 에너지대의 전자 플럭스가 증가하는 현상이 나타남이 관측되었다. 이러한 Relativistic Electron Events (REE) 가속 기작의 주요 후보로 Ultra-Low Frequency(ULF)와 whistler 파동의 역할이 제시되어왔다. 본 연구에서는 1997부터 1999년에 발생한 대표적인 자기 폭풍들을 선택하여, 상대론적 전자 플럭스가 증가한 경우, 감소한 경우 그리고 변화가 크게 나타나지 않는 경우의 세 가지로 분류하여 보았다. 각각의 event들에 대해 CANOPUS 지상자기장 관측소에서 얻은 지자기 값을 이용하여 위 각각의 세 경우에 대해 ULF 파동의 크기 변화를 비교해 보았다. 그리고 똑같은 자기 폭풍 현상에서 POLAR 위성의 관측 값을 이용하여 whistler 영역의 파동 강도를 살펴보았다. 또한 자기 폭풍과 REE, 그리고 ULF의 변화가 L-shell값과 어떤 관련이 있는지도 알아본다.

• Journal of the Korean Magnetics Society
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• v.5 no.4
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• pp.304-308
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• 1995

In order to measure magnetic field difference, we have constructed a fluxgate magnetometer which is based on the measurement of apparent coreci ve field strength from the magnetizing current of two sensors. 'Co-based amorphous ribbon, which has square shape of ac hysteresis loop, was used as core material. Two sensors have 315 turns of the primary and the secondary windings respectively, and core size of 2 mm wide and 30 mm long. The primary windings are connected parallel to measure external magnetic field difference and the secondary windings serieally for the averaged magnetic induction of the cores. The constructed magnetometer could measure magnetic field difference with sensitivity of $1.6{\times}10^{6}V/T$ and resolution of 1 nT at 1 Hz bandwidth.

• Journal of Astronomy and Space Sciences
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• v.23 no.3
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• pp.217-226
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• 2006

We report three sawtooth oscillation events observed at geosynchronous orbit where we find quasi-periodic (every 2-3 hours) sudden flux increases followed by slow flux decreases at the energy levels of ${\sim}50-400keV$. For these three sawtooth events, we have examined variations of the outer boundary of the outer radiation belt. In order to determine L values of the outer boundary, we have used data of relativistic electron flux observed by the SAMPEX satellite. We find that the outer boundary of the outer radiation belt oscillates periodically being consistent with sawtooth oscillation phases. Specifically, the outer boundary of the outer radiation belt expands (namely, the boundary L value increases) following the sawtooth particle flux enhancement of each tooth, and then contracts (namely, the boundary L value decreases) while the sawtooth flux decreases gradually until the next flux enhancement. On the other hand, it is repeatedly seen that the asymmetry of the magnetic field intensity between dayside and nightside decreases (increases) due to the dipolarization (the stretching) on the nightside as the sawtooth flux increases (decreases). This implies that the periodic magnetic field variations during the sawtooth oscillations are likely responsible for the expansion-contraction oscillations of the outer boundary of the outer radiation belt.

• Proceedings of the Korean Magnestics Society Conference
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• 1996.10a
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• pp.114-115
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• 1996

• Proceedings of the Korean Magnestics Society Conference
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• 2015.05a
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• pp.169-170
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• 2015

• Proceedings of the Korean Magnestics Society Conference
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• 2011.12a
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• pp.64-65
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• 2011

• Journal of the Korean Magnetics Society
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• v.22 no.2
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• pp.45-48
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• 2012

Feed-back type 3-axis flux-gate magnetometer using Co-based amorphous ribbon (Metglass$^{(R)}$2714A) was constructed in this work. Measuring range of magnetic field and frequency were ${\pm}100\;{\mu}T$ and dc~10 Hz respectively. For the interface to computer, microcontroller and 24 bit ADC (Analog to Digital Converter) were employed and resolution of digital output was 0.1 nT. Magnetometer noise of analog output was 5 pT/$\sqrt{Hz}$ at 1 Hz. Digital output of the magnetometer showed linearity of $1{\times}10^{-4}$ and the offset drift was smaller than 0.2 nT during 1 h.

• Journal of the Korean Magnetics Society
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• v.23 no.3
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• pp.94-97
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• 2013

Orthogonal fluxgate sensor was fabricated with cylinder-shaped NiZn ferrite core, Cu wire through the core and pickup coil wound on the core, and the bias current effect on the output sensitivity of it was investigated. The output ($$\sim_\sim$$ sensitivity) of the sensor was largely dependent on the operation frequency, and the tendency of sensor output was similar to that of the impedance of pickup coil. The maximum output was obtained by adding the DC bias current of which value was over 50% of the excitation current. The output was saturated when the DC bias current was larger than 50% of the excitation current.

• Proceedings of the Korean Magnestics Society Conference
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• 2009.05a
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• pp.224-225
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• 2009

• Proceedings of the Korean Magnestics Society Conference
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• 2009.05a
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• pp.208-209
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• 2009