• 한국지구과학회지
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• 제33권2호
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• pp.170-182
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• 2012

본 연구의 목적은 행성운동 법칙에 관한 케플러의 귀추적 사고를 도입한 학습자료를 개발하고 이를 고등학교 수업에 적용하여 학생들의 귀추적 추론을 밝히고자 하는 것이다. 이를 위하여 태양의 자기장, 피겨 스케이터의 각운동량 보존, 케플러의 정다면체 이론을 포함한 제시문과 과제문항을 개발하였다. 본 연구의 대상은 과학고등학교 학생 79명과 일반계 고등학교 학생 83명이었고 과제문항에 대한 응답을 비교 분석하여 학생들의 추론 전략 유형과 특성을 논의하였다. 본 연구의 결과, 학생들은 태양의 자기장에 대한 케플러의 생각을 근거로 화성의 운동에 대하여 불완전 유비귀추, 유비귀추, 자료의 재구성 전략을 사용하여 추론하였다. 케플러 제2법칙에 대한 귀추적 추론에서는 불완전 유비귀추, 유비귀추, 모델 구성 및 조작 귀추 등이 나타났다. 이와 관련하여 피겨 스케이터 유비 자체가 학습자들에게 대안개념을 유발할 수 있으므로 실제 수업에서 좀 더 구체적인 설명이 요구됨을 알 수 있었다. 또한 케플러 제3법칙에 대해서는 특히 정다면체 개념과 기존의 알고 있는 지식을 통합하는 개념적 결합 전략을 사용하여 추론한 경우도 나타났다. 적절한 유비귀추를 보여준 과학고 학생의 비율이 일반고 학생보다 여러 과제에서 더 높게 나타난 반면 일반고 학생은 과학고 학생에 비하여 불완전 유비귀추를 더 많이 보여주었다. 본 연구는 케플러의 귀추적 사고를 모델링하여 가설을 형성하는 과정에서 발휘되는 귀추전략을 밝힘으로써 이와 관련한 수업에서 구체적인 방안을 찾는데 근거 자료가 될 것이다.

• 천문학회보
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• 제35권1호
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• pp.27.2-27.2
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• 2010

We have studied the formation of coronal holes (CHs) associated with halo CMEs. For this study, we used multi-wavelength data from Yohkoh Soft X-ray Telescope (SXT), GOES Soft X-ray Imager (SXI), SOHO EIT 195 ${\AA}$, SOHO MDI magnetogram, MLSO He I 10830 ${\AA}$, and BBSO H-alpha. The CHs are characterized by open magentic field regions with low emission, density, and temperature and their open fields drive high speed solar winds which cause geomagnetic storms. So far, the formation and the evolution of CHs are not well understood. The formation of the dark region associated with the eruption of a CME is well known as "coronal dimming" which may be caused by the mass depletion near the CME footpoint. It is different from a typical CH since it persists for only one or two days. In this study, we present three cases that show the formation of coronal holes which are associated with three halo CMEs: 1) 2000 Jul 14, 2) 2003 Oct 28, 3) 2005 May 13. In the first case, hot plasma was ejected during a weak eruption and then filled out the pre-existing CH. After the halo CME occurred, the hot plasma region becomes a CH again. In the second and the third cases, we found newly formed CHs just after their associated CMEs. All three coronal holes are associated with strong flares and persist over 3 days until they disappeared by the solar rotation. Examining the MDI magnetograms, we found that the magnetic polarity of each CH region has one polarity. Based on these results, we suggest that the coronal holes can be formed by the CMEs and they should be distinguished from the coronal dimming.

• 천문학회보
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• 제36권2호
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• pp.89.1-89.1
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• 2011

We have investigated a coronal jet near the limb on 2010 June 27 by Hinode/X-Ray Telescope (XRT), EUV Imaging Spectrograph (EIS), Solar Optical Telescope (SOT), SDO/Atmospheric Imaging Assembly (AIA), and STEREO. From EUV (AIA and EIS) and soft X-ray (XRT) images we identify the erupting jet feature in cool and hot temperatures. It is noted that there was a small loop eruption in Ca II images of the SOT before the jet eruption. Using high temporal and multi wavelength AIA images, we found that the hot jet preceded its associated cool jet. The jet also shows helical-like structures during the rising period. According to the spectroscopic analysis, the jet structure changes from blue shift to red one with time, implying the helical structure of the jet. The STEREO observation, which enables us to observe this jet on the disk, shows that there was a dim loop associated with the jet. Comparing the observations from the AIA and STEREO, the dim loop corresponds to the jet structure which implies the heated loop. Considering that the structure of its associated active region seen in STEREO is similar to that in AIA observed 5 days before, we compared the jet morphology on the limb with the magnetic fields extrapolated from a HMI vector magnetogram observed on the disk. Interestingly, the comparison shows that the open field corresponds to the jet which is seen as the dim loop in STEREO. Our observations (XRT, SDO, SOT, and STEREO) are well consistent with the numerical simulation of the emerging flux reconnection model.

• 한국지구과학회지
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• 제25권7호
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• pp.604-614
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• 2004

경기도 이천에서 2002년 7월부터 12까지 총 6개월 동안 측정된 지자기 3성분 자료를 이용하여 일별 각 성분의 스펙트럼, 지자기 전달함수의 크기, 위상, 오차 등을 계산하였다. 지자기 스펙트럼은 관측기간 동안 태양활동에 의한 무작위적 강약이 반복되는 형태를 보여주었고, 유의미한 시간적 변동은 존대하지 않았다. 지자기 전달함수의 크기, 위상, 오차의 경우, 주기 100초 이하와 주기 1000초 이상에서 부분적으로 무작위적인 경향을 확인할 수 있었으나, 시간에 따른 증감추세 없이 대체로 안정적인 값을 보였다. 이와 더불어, 전기장의 P$_{1}\;^{0}$ 소스(zonal harmonics) 가정을 통하여 시간에 따른 근사적인 겉보기 전기비저항의 변동을 조사하였는데, 근사된 전기비저항의 변화는 지각의 자체적인 물성 변화보다는 수평 자기장 성분의 시간적 강약에 지배적임을 확인할 수 있었다.

• Progress in Superconductivity
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• 제14권1호
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• pp.66-70
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• 2012

Superconductor flywheel energy storage system (SFESs) is an electro-mechanical battery with high energy storage density, long life, and good environmental affinity. SFESs have been developed for application to a regenerative power of train, the storage of distributed power sources such as solar and wind power, and a power quality improvement. As superconductor bearing is completely passive, it is not necessary to control a system elaborately but accurate analysis in mechanical properties of the HTS bearing is very important for application to SFESs. Stiffness and damping properties are the main index for evaluation the capacity of HTS bearings and make it possible to adjust rotordynamic properties while operating the rotor-bearing system. The superconductor bearing consists of a stator containing single grain YBCO bulks, a ring-type permanent magnet rotor with a strong magnetic field that can reach the bulk surface, and a bearing support for assembly to SFESs frame. In this study, we investigated the stiffness and damping properties of superconductor bearings in 35 kWh SFESs. Finally, we found that 35 kWh superconductor bearing has uniform stiffness properties depend on the various orientations of rotor vibration. We discovered total damping coefficient of superconductor bearing is affected by not only magnetic damping in superconductor bulk but also external damping in bearing support. From the results, it is confirmed that the conducted evaluation can considerably improve energy storage efficiency of the SFESs, and these results can be used for the optimal capacity of superconductor bearings of the SFESs.

• 전기학회논문지
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• 제60권5호
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• pp.955-964
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• 2011

In renewable energy system such as flywheel energy storage system, wind power and solar power, the motor/generator is the important key for offering the electric energy to the electric loads. For example, the heavy and large flywheel is rotated by electromagnetic torque of pemanent magnet synchronous motor (PMSM) and, in case of a breakdown of electric current, the PMSM used as generator supplies electric energy for the various electric utilities using mechanical rotation energy of the flywheel. Thus, design of a motor/generator should be performed in effort to reduce cogging torque and electromagnetic loss for high efficiency. In our paper, a slotless permanent magnet synchronous motor/generator (SPMSM/G) with output power 15kW at the rotor speed 18000rpm is designed from electromagnetic analysis and dynamic performance analysis. In analytical approach, design parameters such as back electro-motive force (back EMF), inductance and electromagnetic torque are derived from analytical method which is one of the electromagnetic analysis method. And using the design parameters, this paper deal with system design considering the driving characteristics and electric load in required power. Finally, the analytical results are verified by the experiment and finite element method (FEM).

• 천문학회보
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• 제36권1호
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• pp.35.2-35.2
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• 2011

We have investigated a coronal jet near the limb on 2010 June 27 by Hinode/X-Ray Telescope (XRT), EUV Imaging Spectrograph (EIS), SDO/Atmospheric Imaging Assembly (AIA), and STEREO. From EUV (AIA and EIS) and soft X-ray (XRT) images we identify the erupting jet feature in cool and hot temperatures. Using the high temporal and multi wavelength AIA images, we found that the hot jet preceded its associated cool jet and their structures are well consistent with the numerical simulation of the emerging flux-reconnection model. From the spectroscopic analysis, we found that the jet structure changes from blue shift to red one with time, which may indicate the helical structure of the jet. The STEREO observation, which enables us to observe this jet on the disk, shows that there was a dim loop associated with the jet. On the other hand, we found that the structure of its associated active region seen in STEREO is similar to that in AIA observed 5 days before. Based on this fact, we compared the jet morphology on the limb with the magnectic fields extrapolated from a HMI vector magnetogram of this active region observed on the disk. Interestingly, the comparison shows that the open and closed magnetic field configuration correspond to the jet and the dim loop, respectively, as the Shibata's jet model predicted.

• 천문학회보
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• 제43권2호
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• pp.45.3-46
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• 2018

Oscillations in a sunspot are easily detected through the Doppler velocity observation. Although the sunspot oscillations look erratic, the wavelet analysis show that they consist of successive wave packets which have strong power near three or five minutes. Previous studies found that 3-min oscillation at the chromosphere is a visual pattern of upward propagating acoustic waves along the magnetic field lines. Resent multi-height observations help this like vertical study, however, we also focus on horizontal facet to extend three dimensional understand of sunspot waves. So, we investigate a fragmented sunspot expected to have complex wave profiles according to the positions in the sunspot observed by the Fast Imaging Solar Spectrograph. We choose 4 points at different umbral cores as sampling positions to determine coherence of oscillations. The sets of cross-correlation with three and five minutes bandpass filters during a single wave packet reveal interesting results. Na I line show weak correlations with some lags, but Fe I and Ni I have strong correlations with no phase difference over the sunspots. It is more remarkable at Ni I line with 3-min bandpass that all sets of cross-correlation look like the autocorrelation. We can interpret this as sunspot oscillations occur spontaneously over a sunspot at photosphere but not at chromosphere. It implies a larger or deeper origin of 3-min sunspot oscillation.

• 한국진공학회:학술대회논문집
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• 한국진공학회 2011년도 제41회 하계 정기 학술대회 초록집
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• pp.146-147
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• 2011

Processing a large area substrate for liquid crystal display (LCD) or solar panel applications in a capacitively coupled plasma (CCP) reactor is becoming increasingly challenging because of the size of the substrate size is no longer negligible compared to the wavelength of the applied radio frequency (RF) power. The situation is even worse when the driving frequency is increased to the Very High Frequency (VHF) range. When the substrate size is still smaller than 1/8 of the wavelength, one can obtain reasonably uniform process results by utilizing with methods such as tailoring the precursor gas distribution by adjustingthrough shower head hole distribution or hole size modification, locally adjusting the distance between the substrate and the electrode, and shaping shower head holes to modulate the hollow cathode effect modifying theand plasma density distribution by shaping shower head holes to adjust the follow cathode effect. At higher frequencies, such as 40 MHz for Gen 8.5 (2.2 m${\times}$2.6 m substrate), these methods are not effective, because the substrate is large enough that first node of the standing wave appears within the substrate. In such a case, the plasma discharge cannot be sustained at the node and results in an extremely non-uniform process. At Applied Materials, we have studied several methods of modifying the standing wave pattern to adjusting improve process non-uniformity for a Gen 8.5 size CCP reactor operating in the VHF range. First, we used magnetic materials (ferrite) to modify wave propagation. We placed ferrite blocks along two opposing edges of the powered electrode. This changes the boundary condition for electro-magnetic waves, and as a result, the standing wave pattern is significantly stretched towards the ferrite lined edges. In conjunction with a phase modulation technique, we have seen improvement in process uniformity. Another method involves feeding 40 MHz from four feed points near the four corners of the electrode. The phase between each feed points are dynamically adjusted to modify the resulting interference pattern, which in turn modulate the plasma distribution in time and affect the process uniformity. We achieved process uniformity of <20% with this method. A third method involves using two frequencies. In this case 40 MHz is used in a supplementary manner to improve the performance of 13 MHz process. Even at 13 MHz, the RF electric field falls off around the corners and edges on a Gen 8.5 substrate. Although, the conventional methods mentioned above improve the uniformity, they have limitations, and they cannot compensate especially as the applied power is increased, which causes the wavelength becomes shorter. 40 MHz is used to overcome such limitations. 13 MHz is applied at the center, and 40 MHz at the four corners. By modulating the interference between the signals from the four feed points, we found that 40 MHz power is preferentially channeled towards the edges and corners. We will discuss an innovative method of controlling 40 MHz to achieve this effect.

• Journal of Astronomy and Space Sciences
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• 제14권2호
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• pp.275-285
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• 1997

1989년 2월에 일본의 우주과학연구소(ISAS: Institute of Space and Astronautical Science)에서 발사한 과학위성 EXOS-D의 전기장 측정기와 지자기 자오선 동경 190/210 선상에 위치하고 있는 17개의 지상자력계들로부터 1994년 11월 09일 18시 50분부터 약 20분에 걸쳐 Pi 2 파동이 검출되었다. 우리가 이용한 지상자력계는 지자기 경도는 동경 185.02에서 동경 269.36사이, 지자기 위도는 -37.09에서 65.67사이에, L값은 1.00에서 5.89사이에 위치하고 있다. 또한 같은 시각에 또 다른 위성 ETS-VI의 자기장 측정기의 자료와 지상의 Kakioka(지자기 동경 208.00, 지자기 위도 26.70), Hermanus(지자기 동경 82.97, 지자기 위도 -33.78) 지상자력계의 자료도 함께 사용하여 비교하여 보았다. Pi 2 파동의 주파수를 알아내기 위하여 FFT를 이용하였으며, L값이 2.35인 EXOS-D 위성과 지상자력계들에서는 주파수가 약 25mHz에서 최대 값을 보였으나, L값이 6.60인 ETS-VI위성에서는 같은 주파수가 검출되지 않았다. 또한 지상자력계 중에서 MUT 지상자력계의 자료를 기준으로 하여 위성들과 나머지 지상자력계들간의 상관관계, 위상 차를 조사하여, 발견된 Pi 2 파 동 현상이 플라즈마구 내에서 형성된 공동(cavity) mode에 의한 현상임을 알 수 있었다.