Bach ground: The correlation between sunspot proper motion and flares has been investigated for a long time (e.g. Antalova, 1965, Gesztelyi, 1984). The.

Slides:



Advertisements
Similar presentations
The flare-CME relationship – determining factors (if any!) Sarah Matthews, Lucie Green, Hilary Magee, Louise Harra & Len Culhane MSSL, University College.
Advertisements

Investigating the Origin of the Long-Duration High- Energy Gamma-Ray Flares Gerry Share, Jim Ryan and Ron Murphy (in absentia) Steering Committee Overseer.
RHESSI observations of LDE flares – extremely long persisting HXR sources Mrozek, T., Kołomański, S., Bąk-Stęślicka, U. Astronomical Institute University.
Chapter 2. Concepts of Motion
Chapters E12 (and E13) The Electromagnetic Field.
Flare energy release and wave dynamics in nearby sunspot Solar and Stellar Flares, Observations, simulations and synergies June , 2013, Prague,
11/26/081 AUTOMATIC SOLAR ACTIVITY DETECTION BASED ON IMAGES FROM HSOS NAOC, HSOS YANG Xiao, LIN GangHua
Estimating the magnetic energy in solar magnetic configurations Stéphane Régnier Reconnection seminar on Thursday 15 December 2005.
Hot Precursor Ejecta and Other Peculiarities of the 2012 May 17 Ground Level Enhancement Event N. Gopalswamy 2, H. Xie 1,2, N. V. Nitta 3, I. Usoskin 4,
TRACE and RHESSI observations of the failed eruption of the magnetic flux rope Tomasz Mrozek Astronomical Institute University of Wrocław.
Study of Magnetic Helicity Injection in the Active Region NOAA Associated with the X-class Flare of 2011 February 15 Sung-Hong Park 1, K. Cho 1,
Identification and Analysis of Magnetic Substorms Patricia Gavin 1, Sandra Brogl 1, Ramon Lopez 2, Hamid Rassoul 1 1. Florida Institute of Technology,
The Solar Cycle for seeing the sun exhibit. The Sun’s Magnetic Field The magnetic field on the sun is produced by the flow of electrically charged ions.
RHESSI 2003 October 28 Time Histories Falling fluxes following the peak Nuclear/511 keV line flux delayed relative to bremsstrahlung Fit to 511 keV line.
East-West Asymmetry of the Yohkoh Soft X-ray Corona L.W. Acton 1, D.E. McKenzie 1, A. Takeda 1, B.T. Welsch 2,and H.S. Hudson 2,3 1 Montana State University,
Intense Flares Without Solar Energetic Particle Events N. V. Nitta (LMSAL), E. W. Cliver (AFRL), H. S. Hudson (UCB) Abstract: We study favorably located.
Hard X-ray footpoint statistics: spectral indices, fluxes, and positions Pascal Saint-Hilaire 1, Marina Battaglia 2, Jana Kasparova 3, Astrid Veronig 4,
One mask to group them all, One code to find them, One file to store them all, And in a structure bind them. William (Tolkien) Simpson m.
High-latitude activity and its relationship to the mid-latitude solar activity. Elena E. Benevolenskaya & J. Todd Hoeksema Stanford University Abstract.
RHESSI OBSERVATIONS OF FLARE FOOTPOINTS AND RIBBONS H. Hudson and M. Fivian (SSL/UCB)
Observations of the failed eruption of the magnetic flux rope – a direct application of the quadrupolar model for a solar flare Tomasz Mrozek Astronomical.
Rapid Changes in the Longitudinal Magnetic Field Associated with the July gamma -ray Flare Vasyl Yurchyshyn, Haimin Wang, Valentyna Abramenko,
The Change of Magnetic Inclination Angles Associated with Flares Yixuan Li April 1,2008.
Reverse Drift Bursts in the GHz Band and their Relation to X-Rays František Fárník and Marian Karlický Astronomical Institute Academy of Sciences.
Solar Activities and Halloween Storms Ahmed Hady Astronomy Department Cairo University, Egypt.
Magnetic Shear in Two-ribbon Solar Flares Yingna Su 1,2 Advisors: Leon Golub 1, Guangli Huang 2 Collaborators: A. A. Van Ballegooijen 1, E. E. Deluca 1,
Coronal Ejecta in October - November of 2003 and predictions of the associated geomagnetic events 1 Big Bear Solar Observatory, New Jersey Institute of.
Helicity on the Sun: What is it good for anyway? Slide 1 of
Free Magnetic Energy in Solar Active Regions above the Minimum-Energy Relaxed State (Regnier, S., Priest, E.R ApJ) Use magnetic field extrapolations.
Study of magnetic helicity in solar active regions: For a better understanding of solar flares Sung-Hong Park Center for Solar-Terrestrial Research New.
Kinetic and Magnetic Helicities of Solar Active Regions Ram Ajor Maurya, Ashok Ambastha And Vema Reddy Udaipur Solar Observatory Physical Research Laboratory,
Detection of Emerging Sunspot Regions in the Solar Interior Stathis Ilonidis, Junwei Zhao, and Alexander Kosovichev Stanford University LoHCo Workshop.
The nature of impulsive solar energetic particle events N. V. Nitta a, H. S. Hudson b, M. L. Derosa a a Lockheed Martin Solar and Astrophysics Laboratory.
EUV vs. B-field Comparisons Yingna Su Smithsonian Astrophysical Observatory Coauthours: Leon Golub, Aad Van Ballegooijen, Maurice Gros. HMI/AIA Science.
Magnetic Structures of Active Regions and their Link to Coronal Mass Ejections Vasyl Yurchyshyn, Big Bear Solar Observatory, Big Bear City, CA 92314,
Thomas Zurbuchen University of Michigan The Structure and Sources of the Solar Wind during the Solar Cycle.
AOS 101 Weather and Climate Lisha M. Roubert University of Wisconsin-Madison Department of Atmospheric & Oceanic Sciences.
The Sun. Solar Prominence Sun Fact Sheet The Sun is a normal G2 star, one of more than 100 billion stars in our galaxy. Diameter: 1,390,000 km (Earth.
Flares in and their associations with CMEs N.V. Nitta, J.P.Wuelser, M. J. Aschwanden, J. R. Lemen (LMSAL), D. M. Zarro (Adnet, Inc.)
Quick changes of photospheric magnetic field during flare-associated surges Leping Li, Huadong Chen, Suli Ma, Yunchun Jiang National Astronomical Observatory/Yunnan.
The Relation between Soft X-ray Ejections and Hard X-ray Emission on November 24 Flare H. Takasaki, T. Morimoto, A. Asai, J. Kiyohara, and K. Shibata Kwasan.
Micro-Flare and High-Speed Down-Flow observed with VTT R. Kano(1), Y. Katsukawa(1), Y. Kitakoshi(2), T. Shimizu(3), S. Tsuneta(1) and V. Martinez Pillet(4)
Locating the solar source of 13 April 2006 Magnetic Cloud K. Steed 1, C. J. Owen 1, L. K. Harra 1, L. M. Green 1, S. Dasso 2, A. P. Walsh 1, P. Démoulin.
RHESSI and Radio Imaging Observations of Microflares M.R. Kundu, Dept. of Astronomy, University of Maryland, College Park, MD G. Trottet, Observatoire.
The quantitative analysis of the spiral chirality of penumbral filament 1 Helicity Thinkshop on Solar Physics, Oct. 2013, Beijing Liu J.H., Su J.T. et.
1 THE RELATION BETWEEN CORONAL EIT WAVE AND MAGNETIC CONFIGURATION Speakers: Xin Chen
SHINE SEP Campaign Events: Long-term development of solar corona in build-up to the SEP events of 21 April 2002 and 24 August 2002 A. J. Coyner, D. Alexander,
ASAI Ayumi Kwasan Observatory, Kyoto University July 12, Evolution of Flare Ribbons and Energy Release.
Analysis Magnetic Reconnection in Solar Flares: the Importance of Spines and Separators Angela Des Jardins 1, Richard Canfield 1, Dana Longcope 1, Emily.
NoRH Observations of RHESSI Microflares M.R. Kundu, Dept. of Astronomy, University of Maryland, College Park, MD E.J.Schmahl, Dept. of Astronomy, University.
SH 51A-02 Evolution of the coronal magnetic structures traced by X-ray and radio emitting electrons during the large flare of 3 November 2003 N.Vilmer,
1. Twist propagation in Hα surges Patricia Jibben and Richard C. Canfield 2004, ApJ, 610, Observation of the Molecular Zeeman Effect in the G Band.
KASI Low atmospheric reconnections associated with an eruptive flare Yong-Jae Moon(1), Jongchul Chae(2), Young-Deuk Park(1) 1: Korea Astronomy and.
Solar seminor: 4 Oct (1)Eruption of a multiple-turn helical magnetic flux tube in a large flare : Evidence for external and i ternal reconnection.
Today’s Papers 1. Flare-Related Magnetic Anomaly with a Sign Reversal Jiong Qiu and Dale E. Gary, 2003, ApJ, 599, Impulsive and Gradual Nonthermal.
Uniform motion, slope and speed
Direct Spatial Association of an X-Ray Flare with the Eruption of a Solar Quiescent Filament Gordon D. Holman and Adi Foord (2015) Solar Seminar on July.
Moving Magnetic Features as Prolongation of Penumbral Filaments The Astrophysical Journal, 632: , 2005 October 20. Sainz Dalda 1 Telescope Heliographique.
What we can learn from active region flux emergence David Alexander Rice University Collaborators: Lirong Tian (Rice) Yuhong Fan (HAO)
High Spatial Resolution Observations of Pores and the Formation of a Rudimentary Penumbra G. Yang, Y.Xu, H.Wangm and C.Denker 2003, ApJ, 597, 1190.
Sunspot Group Evolution and Flare Forecasting
Studies on Twisted Magnetic Flux Bundles
CH29: The Sun Mrs. Kummer, 2016.
Spatial Modes of Salinity and Temperature Comparison with PDO index
The CME-Flare Relationship in Homologous Eruptive Events
Teriaca, et al (2003) ApJ, 588, SOHO/CDS HIDA/DST 2002 campaign
Preflare State Rust et al. (1994) 太陽雑誌会.
High-cadence Radio Observations of an EIT Wave
Flare Ribbon Expansion and Energy Release
-Short Talk- The soft X-ray characteristics of solar flares, both with and without associated CMEs Kay H.R.M., Harra L.K., Matthews S.A., Culhane J.L.,
Presentation transcript:

Bach ground: The correlation between sunspot proper motion and flares has been investigated for a long time (e.g. Antalova, 1965, Gesztelyi, 1984). The fast motion often connected with flare activity. The acceleration in the proper motion is correlated in time to the occurence of flares in the neighborhood of the spots. Dezs¨o et al. (1980) found that some sunspots showed abrupt change in both speed and direction of proper motion in the phase of flare maximum. The very striking change in position and shape of sunspots close to a flare during the impulsive phase was found by Anwar et al. (1993), and explained as the evidence of energy release location. It has been suggested that proper motion of sunspot is regarded as a flare precursor, since the proper motion led to magnetic energy build up. Many major flares took place on a region where their spots show large proper motion (Ambastha & Bhatnagar, 1988; Dezs¨o et al.,1980). It is clear that any change in proper motion of sunspots may have close correlation with flare occurence. This implies the the flare prediction could be made by measuring the spot proper motion However, precursor events, especially in a few hours before the flare onset has not been known. The precursor mechanism triggering flare in the short period before flare onset is still unknown. In studying the proper motion of sunspot in short time scale before flare onset, we seek to any change in spot motion just before flare. This should give us the preliminary indicator in predicting the flare onset, and may allow us to find the timing of energy build up or release. Change in Sunspot Proper Motion and Its Relation to Flare Onset C.Y. Yatini (LAPAN) and Y. Suematsu (NAOJ) ABSTRACT: From the detailed measurements of motion of sunspots in six active regions, we found that some spots, which are located on flaring area, underwent a particular motion when compared with other spots in the same active region. These spots showed a 'turn' in their moving direction before flare started. The change in motion started in 0.5 to 2.5 hours before flare onset. We found the relation that if the spot shows a 'particular‘ motion, a flare occurs on this particular spot region. On the other hand, any sunspots in non-flaring active region do not show peculiar motion. In some cases, the particular spots also show the motion consistent with a rising emerging flux tube in which pair of spots move away from each other. It is likely that the peculiar motion of spots implies the rising motion of flux tube perturbed by unknown reason. From this study, we expect that SOLAR-B/SOT will be able to reveal the detailed relation between the sunspot motion, related magnetic activity and flare onset, making a short term prediction of flare occurrence possible. P60 Method of Data Analysis Tracking spots  Local Cross-correlation ; - forward tracking - backward tracking  Spot’s center of gravity to get reliable result, since the spot displacement is small and the image is affected by variable atmospheric seeing. NOAA 8100 on Nov 3, 1997 On 1997 November 3, the active region NOAA 8100 produced an SB/C8.6 flare. In the tracking of spots movement, we divided this active region into 3 groups (labeled A, B and C). Each spots movement is measured against its group. In group A the positive polarity spots are spots 2, 3, 5, 6, 7, 8, 9, and 10; in group B are nos 5 and 6; in group C is spot 2. Others than those are negative ones. Spots A2, C9 and C10 were appeared at about 01:30 UT or about 2.5 hours before flare onset. Solid vertical lines represent flare onset time. Arrows show the timing of the disturbance in spots movement. Active region NOAA 7912 on October 13, Spots are marked with number in the tracking of their movement. The ensemble of spots group (box no 1) is used as the reference. The displacement plots of spot no 2 (dotted line), 4 (dashed), 5 (solid), 6 (dash dot), 10 (dash dot dot) and 11(long dash). Solid vertical line represents the flare onset time. Arrows show the ’turning’ time of spot 5. Left is the result of forward, right is of backward tracking. Active region NOAA 8395 (fig 17) produced a 3N/X3.3 class flare on November 28, We divided the tracking of spots in two parts. In part A, we measured the spots displacement with the reference of area A. In this area spots no A8, A9, and A10 are negative polarity spots, while the others are positive. In the second part (B), we measured the spots outside of area A using spot A2 as the reference. NOAA 8123 on 1997 December 18: The spots displacement in non flaring period of active region also analyzed as well as the flaring active region. The result is used as the comparison of the movement of spots in flaring region. We used area 1, which including spots 2, 3, and 4, as the reference. There were three spots in the boxed area, and labeled as no All spots is negative polarity. The spot located on west side of this box has positive polarity. In this figure, the spots kept their moving direction during the observation. The spot which has biggest displacement is spot no 2, but it did not show any remarkable change in its movement. Conclusion and Discussion: We have studied the spots displacement in some active regions before flare onset. In the result of the measurement we bring a new view about the proper motion of spots in a short term scale before flare onset. From the observation of spots movement in active regions, we found that some spots, which were located beneath Hα flare ribbon footpoints, underwent a particular motion compared with other spots in the same active region. They moved in different pattern. These spots underwent a disturbance in their moving direction before the flare started. The disturbance could be either in the east - west or the north - south direction. It started 2 hours to 30 minutes before the flare onset. This phenomenon always occurred in all the flaring active regions we studied in this paper. The spots proper motion in short time scale before flare onset give us a new view in finding the flare precursor. This finding lead to the suggestion that if a sunspot shows a ’peculiar’ motion different from other sunspots in the same active region, a flare should occur on its sunspot area a few hours later or so. On the other hand, from the GOES X-ray plots, we found no remarkable sign was observed that can be used as the precursor of flares. They show no remarkable sign before flare onset. We suggest that the proper motion is a better indicator for flare than the X-ray intensity. As the results, we suggest that in the future, the disturbance in proper motion of spots in active region might allow us to predict the flare occurrence in short time scale. We expect that SOLAR-B/SOT will be able to reveal the detailed relation between the sunspot motion, related magnetic activity and flare onset, making a short term prediction of flare occurrence possible. Data were provided by Solar Flare Telescope, Mitaka, NAOJ, data selection rule is: Continuous data (images) in order of few minutes before flare onset Continuous data (images) in order of few minutes before flare onset No flare erupted in the same active region before selected flare No flare erupted in the same active region before selected flare Data sets used in this study.