• 제목/요약/키워드: Solar magnetic field

검색결과 249건 처리시간 0.029초

Three-Dimensional Numerical Magnetohydrodynamic Simulations of Magnetic Reconnection in the Interstellar Medium

  • TANUMA SYUNITI;YOKOYAMA TAKAAKI;KUDOH TAKAHIRO;SHIBATA KAZUNARI
    • 천문학회지
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    • 제34권4호
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    • pp.309-311
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    • 2001
  • Strong thermal X-ray emission, called Galactic Ridge X-ray Emission, is observed along the Galactic plane (Koyama et al. 1986). The origin of hot ($\~$7 keV) component of GRXE is not known, while cool ($\~$0.8 keV) one is associated with supernovae (Kaneda et al. 1997, Sugizaki et al. 2001). We propose a possible mechanism to explain the origin; locally strong magnetic fields of $B_{local}\;\~30{\mu}G$ heat interstellar gas to $\~$7 keV via magnetic reconnection (Tanuma et al. 1999). There will be the small-scale (< 10 pc) strong magnetic fields, which can be observed as $(B)_{obs} \;\~3{\mu}G$ by integration of Faraday Rotation Measure, if it is localized by a volume filling factor of f $\~$ 0.1. In order to examine this model, we solved three-dimensional (3D) resistive magnetohydrodynamic (MHD) equations numerically to examine the magnetic reconnect ion triggered by a supernova shock (fig.l). We assume that the magnetic field is Bx = 30tanh(y/20pc) $\mu$G, By = Bz = 0, and the temperature is uniform, at the initial condition. We put a supernova explosion outside the current sheet. The supernova-shock, as a result, triggers the magnetic reconnect ion, and the gas is heatd to > 7 keV. The magnetic reconnect ion heats the interstellar gas to $\~$7 keV in the Galactic plane, if it occurs in the locally strong magnetic fields of $B_{local}\;\~30{\mu}G$. The heated plasma is confined by the magnetic field for $\~10^{5.5} yr$. The required interval of the magnetic reconnect ions (triggered by anything) is $\~$1 - 10 yr. The magnetic reconnect ion will explain the origin of X-rays from the Galactic ridge, furthermore the Galactic halo, and clusters of galaxies.

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전파통신에서의 전리층 역할 (IONOSPHERIC EFFECTS ON THE RADIO COMMUNICATION)

  • 표유선;조경석;이동훈;김은화
    • 천문학논총
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    • 제15권spc2호
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    • pp.21-25
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    • 2000
  • The ionosphere, the atmosphere of the earth ionized by solar radiations, has been strongly varied with solar activity. The ionosphere varies with the solar cycle, the seasons, the latitudes and during any given day. Radio wave propagation through or in the ionosphere is affected by ionospheric condition so that one needs to consider its effects on operating communication systems normally. For examples, sporadic E may form at any time. It occurs at altitudes between 90 to 140 km (in the E region), and may be spread over a large area or be confined to a small region. Sometimes the sporadic E layer works as a mirror so that the communication signal does not reach the receiver. And radiation from the Sun during large solar flares causes increased ionization in the D region which results in greater absorption of HF radio waves. This phenomenon is called short wave fade-outs. If the flare is large enough, the whole of the HF spectrum can be rendered unusable for a period of time. Due to events on the Sun, sometimes the Earth's magnetic field becomes disturbed. The geomagnetic field and the ionosphere are linked in complex ways and a disturbance in the geomagnetic field can often cause a disturbance in the F region of the ionosphere. An enhancement will not usually concern the HF communicator, but the depression may cause frequencies normally used for communication to be too high with the result that the wave penetrates the ionosphere. Ionospheric storms can occur throughout the solar cycle and are related to coronal mass ejections (CMEs) and coronal holes on the Sun. Except the above mentioned phenomena, there are a lot of things to affect the radio communication. Nowadays, radio technique for probing the terrestrial ionosphere has a tendency to use satellite system such as GPS. To get more accurate information about the variation of the ionospheric electron density, a TEC measurement system is necessary so RRL will operate the system in the near future.

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북쪽방향 IMF 조건하에서 발생하는 서브스톰의 통계적 특성 (Some Statistical Characteristics of Substorms Under Northward IMF Conditions)

  • 이지희;이대영;최규철;정연철
    • Journal of Astronomy and Space Sciences
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    • 제26권4호
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    • pp.451-466
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    • 2009
  • 서브스톰(substorm)은 일반적으로 IMF가 남쪽 방향(이하 southward IMF)일 때 발생하기 쉽지만 IMF가 북쪽 방향(이하 northward IMF)일 때도 발생한다. 이 연구에서는 northward IMF 상태일 때 발생하는 서브스톰의 특성을 규명하기 위해 2000년 5월부터 2002년까지의 기간에 발생한 서브스톰을 다루었다. 특히 northward IMF 기간 중 두 번 혹은 그 이상의 서브스톰이 연이어서 발생한 경우에 대한 총 53건의 서브스톰을 선정하였다. 이렇게 선정된 서브스톱에 대해 그 해당 IMF와 태양풍의 통계적 조건을 조사하였다. 또한 자기폭풍(magnetic storm)과의 연관성을 알아보고자 Sym-H의 변화를 조사하였다. 정지궤도에서 자기장의 쌍극자화(magnetic dipolarization) 정도와 고 에너지 입자 발생(energetic particle injection) 강도에 대해서도 조사 하였다. 서브스톰이 발생할 수 있는 에너지 유입의 근원을 알아보기 위해 IMF clock angle를 조사하였다. 이와 같은 조사를 통해 다음과 같은 결과를 얻었다. (1) northward IMF 서브스톰은 태양풍 물리량들이 보편적으로 알려진 평균 값을 가질 때 가장 높은 발생 빈도를 보였다. northward IMF로 바뀐 후 첫 번째로 발생된 서브스톰의 87%, 그 이후의 서브스톰들의 62%가 northward IMF 상태가 지속 된지 두 시간 이내에 발생 하였다. 이것은 곧 2 시간 이상 northward IMF 상태가 지속된 후에도 발생하는 서브스톰이 종종 존재한다는 것을 시사한다. (2) 대부분의 경우 자기폭풍과 독립된 서브스톰 이였으나, 자기폭풍 기간에 발생한 서브스톰의 경우에는 그렇지 않은 서브스톰들과 비교 하였을 때, 그 해당 IMF와 태양풍의 물리량들이 다소 높은 평균 값을 보였다. (3) 약 55%의 서브스톰은 낮지역의 자기장 재결합(dayside reconnection)이 가능 할 정도의 IMF clock angle을 갖는 상태이지만, 나머지 45%의 서브스톰의 경우는 그렇지 않은 것으로 나타났다. 따라서 이런 경우 낮지역 자기장 재결합 이외의 다른 방법에 의한 에너지 유입이 이루어 져야 할 것으로 본다. (4) 또한 많은 경우 정지궤도에서의 자기장의 쌍극자화 정도와 고 에너지 입자 발생 정도가 대체로 약한 것을 확인하였다. 하지만, 일부 이벤트에서는 강한 자기장 쌍극자화와 고 에너지 입자 발생이 나타났다.

SONDRESTROM 비간섭 산란 레이더 자료를 이용한 극지방 전리층의 기후학적 특성 연구 (CLIMATOLOGICAL CHARACTERISTICS OF THE POLAR IONOSPHERE BASED ON THE SONDRESTROM INCOHERENT SCATTER RADAR MEASUREMENTS)

  • 곽영실;안병호
    • Journal of Astronomy and Space Sciences
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    • 제19권1호
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    • pp.75-88
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    • 2002
  • 전리층의 전기 전도도와 전기장을 구함으로써 극지방 전리층의 기후학적 특성을 살펴보았다 이를 위해, 총 109일간의 Sondrestrom 비간섭 산란 레이더 자료를 이용하였다. 전기 전도도와 전기장을 이용하여 전리층 전류 분포를 추정하였고, 구해진 전리층 전류 밀도와 그로 인해 유발되는 지상 지자기 변화를 비교하였다. 또한 지상 지자기 변화(특히, D 성분)에 대한 연자기력선 전류의 효과도 검토되었다. Sondrestrom 상공 전리층에 대한 몇 가지 흥미로운 기후학적 특성을 본 연구로부터 알 수 있었다: (1) 주간의 전기 전도도 분포는 주로 태양 EUV복사에 의한 것이며, 야간에는 미약하다. (2) 극관 영역 전리층의 전기 전도도 분포는, 주간에는 태양 EUV복사에 의한 분포를 보이는 반면, 야간에는 Hall 및 Pedersen 전기 전도도의 시간 평균이 각각 1.6 및 1.2 siemen으로 아주 낮다. (3) 남북 성분 전기장의 최대치가 낮 영역에 나타나는 경향이 있다. 동서 성분 전기장은 Chatanika에 비해 강하다 (4) 동서 성분 전류는 낮 영역에서 강하게 흐른다. 정오 바로 전에 강한 남향 전류가 흐른다. (5) 오로라제트전류와 동시에 관측된 지상 지자기 변화 $({{\Delta}}H)$ 사이에 높은 상관관계를 나타낸다. 하지만 무한판상을 가정한 전류가 크게 과소평가 된다. 또한 ${{\Delta}}H$의 관계보다 더 높게 나타나며, 이것은 연자기력선 전류가 ${\Delta}7$에 영향을 미친다는 것을 의미한다.

Study of Magnetic Helicity Injection in the Active Region NOAA 9236 Producing Multiple CME Events

  • Park, Sung-Hong;Cho, Kyung-Suk;Bong, Su-Chan;Park, Young-Deuk
    • 천문학회보
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    • 제36권2호
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    • pp.84.1-84.1
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    • 2011
  • In this study, we intend to inquire of how the temporal variation and spatial distribution of magnetic helicity injection in a CME-producing solar active region are related to the CME occurrence. We therefore investigate long-term (a few days) variation of magnetic helicity injection in the active region NOAA 9236 which produced multiple CME events. As a result, it is found that a noticeable increase in helicity of negative sign was first made for the first ~1.5 days and then 6 CMEs occurred while the relatively more injection of oppositely signed (positive) helicity was taking place for the next ~2 days. Afterwards, 2 CMEs in the region occurred while a more negative helicity is being injected again compared to a positive helicity. In addition, from helicity flux density maps, we found that the CMEs originated from this active region seem to be involved with the interaction of two magnetic field systems characterized by opposite signs of helicity.

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Stability Analysis of the Magnetic Structures Producing an M6.5 Flare in active region 12371

  • Kang, Jihye;Inoue, Satoshi;Kusano, Kanya;Park, Sung-Hong;Moon, Yong-Jae
    • 천문학회보
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    • 제44권2호
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    • pp.41.1-41.1
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    • 2019
  • The stability analysis of coronal magnetic structures is important for studying the initiation of solar flares and eruptions. In order to understand the flare onset process, we first reconstructed the 3D coronal magnetic structures of active region 12371 with an M6.5 flare using a nonlinear force-free field (NLFFF) model based on vector magnetic fields. The NLFFFs successfully produce the observed sigmoidal structure which is composed of two branches of sheared arcade loops. The stability analysis were examined for three representative MHD instabilities: the kink, the torus, and the double arc instabilities. Our stability analysis shows that the two branches of sheared arcade loops are quite stable against the kink and torus instabilities, but unstable against the double arc instability before the flare occurrence. Finally, we discuss a probable onset process of the M6.5 flare.

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Proton Temperature Anisotropy vs Parallel Beta in the Solar Wind

  • Yoon, Peter H.
    • 천문학회보
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    • 제36권2호
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    • pp.92.2-92.2
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    • 2011
  • In view of the planned NASA's and ESA's Solar Probe Plus and Solar Orbiter missions, respectively, to probe the inner heliosphere and the Sun's corona, it is timely to investigate outstanding problems associated with the solar wind. Among them is the temperature anisotropy problem. As the solar wind expands into the interplanetary space, the density and magnetic field decreases radially, thus leading to temperature anisotropy ($T_{\parallel}{\gg}T_{\perp}$). However, the measured temperature anisotropy can at times be characterized by $T_{\perp}$ > $T_{\parallel}$, while at other times the measured $T_{\parallel}/T_{\perp}$ is much milder than predicted by adiabatic theory. Physical reasons remain poorly understood. This notwithstanding, it is known from plasma physics that for $T_{\perp}$ > $T_{\parallel}$ electromagnetic ion-cyclotron (EMIC) and mirror instabilities are excited, while for $T_{\parallel}$ > $T_{\perp}$, fire-hose instability is excited. By constructing the threshold conditions for various instabilities, one may construct a closure relation that may be useful for modeling the solar wind. In the present paper we discuss theoretical construction of the anisotropy-beta relation by means of quasi-linear theories of these instabilities. The present work complements previous efforts on the basis of linear theory, hybrid simulations, and empirical fits of observations.

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On the Optical Characteristics of Solar X-Ray Telescopes: Possible Relation between Vignetting Effect and Mirror Scattering

  • Shin, Jun-Ho;Sakurai, Takashi
    • 천문학회보
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    • 제36권2호
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    • pp.87.1-87.1
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    • 2011
  • Since early 90's, the solar X-ray telescopes such as Yohkoh SXT and Hinode XRT have observed coronal magnetic structures on the Sun's surface in the range of about $40'{\times}40'$ field-of-view (FOV) covering the full solar disk. Thus it has been stressed by the scientists that the optical structure of solar telescopes should be designed with care for improving the uniformity over a wide FOV. There would be, however, no unique solution in designing the optical system of a telescope for overcoming perfectly the problem of off-axis response variation. As a consequence, the correction of optical imperfectness of telescopes has become an important calibration step that should be performed beforehand when the observed images are to be used for photometric purposes. In particular, a special care should be taken when performing the temperature analysis with thin and thick filters for flaring activities observed at the periphery of the full FOV. From the analyses of both pre-launch calibration and in-flight observation data, the optical characteristics for describing the performance of solar X-ray telescopes, especially in view of their energy dependence, will be introduced and discussed in our presentation.

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Solar and Heliospheric 1.3-year Signals during 1970-2007

  • Hwang, Junga;Cho, Il-Hyun;Park, Yound-Deuk
    • 천문학회보
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    • 제38권2호
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    • pp.92.2-92.2
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    • 2013
  • We revisit the 1.3-year (yr) signals observed on the Sun, in the interplanetary space, and in the Earth's magnetosphere to study the coupling among signals from the three regions for about forty years (1970--2007) covering three solar cycles 21, 22, and 23. For this, we make dynamic spectra of datasets including three different regions. From this, we estimate the peak frequency around 1.3 yr for each region and the corresponding band power. We found that coherent power only appears during 1987-1995 and the coherent behavior is found only in the interplanetary space and Earth, not in the Sun. Although the solar surface magnetic field shows significant power around 1.3 yr, their peak frequencies are statistically different from those of the outer regions, which make us to dismiss the existence of coherence among the three regions. But it is notable that the peaks in band power corresponding to the 1.3-yr period are clearly simultaneous in the interplanetary space and Earth.

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Do Inner Planets Modulate the Space Environment of the Earth?

  • Kim, Jung-Hee;Chang, Heon-Young
    • Journal of Astronomy and Space Sciences
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    • 제31권1호
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    • pp.7-13
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    • 2014
  • Variabilities in the solar wind cause disturbances throughout the heliosphere on all temporal and spatial scales, which leads to changeable space weather. As a view of space weather forecasting, in particular, it is important to know direct and indirect causes modulating the space environment near the Earth in advance. Recently, there are discussions on a role of the interaction of the solar wind with Mercury in affecting the solar wind velocity in the Earth's neighborhood during its inferior conjunctions. In this study we investigate a question of whether other parameters describing the space environment near the Earth are modulated by the inner planets' wake, by examining whether the interplanetary magnetic field and the proton density in the solar wind observed by the Advanced Composition Explorer (ACE) spacecraft, and the geomagnetic field via the Dst index and Auroral Electrojet index (AE index) are dependent upon the relative position of the inner planets. We find there are indeed apparent variations. For example, the mean variations of the geomagnetic fields measured in the Earth's neighborhood apparently have varied with a timescale of about 10 to 25 days. Those variations in the parameters we have studied, however, turn out to be a part of random fluctuations and have nothing to do with the relative position of inner planets. Moreover, it is found that variations of the proton density in the solar wind, the Dst index, and the AE index are distributed with the Gaussian distribution. Finally, we point out that some of properties in the behavior of the random fluctuation are to be studied.