csi 769/astr 769 topics in space weather fall 2005 lecture 03 sep. 13, 2005 solar eruptions: flares...

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CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections •Aschwanden, “Physics of the Solar Corona” •Chap. 16, P671-702, Flare Plasma Dynamics •Chap. 17, P703-737, Coronal Mass Ejections (CMEs) •Chap. 10, P407-463, Magnetic Reconnection

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Page 1: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CSI 769/ASTR 769 Topics in Space Weather Fall 2005Lecture 03 Sep. 13, 2005

Solar Eruptions: Flares and Coronal Mass Ejections

•Aschwanden, “Physics of the Solar Corona”•Chap. 16, P671-702, Flare Plasma Dynamics•Chap. 17, P703-737, Coronal Mass Ejections (CMEs)•Chap. 10, P407-463, Magnetic Reconnection

Page 2: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of
Page 3: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

8010 + 17:17 17:40 18:03 G12 5 XRA 1-8A X17.0 2.6E00 0808

Page 4: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

3-day Solar-Geophysical Forecast issued Sep 12 at 22:00 UTC Solar Activity Forecast: Solar activity is expected to be moderate to high

http://www.sec.noaa.gov

Page 5: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Magnetogram on Sep. 08 Sep. 12

Page 6: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

What is a solar flare?

•A solar flare is a sudden brightening of a part of the chromosphere and/or corona, by traditional definition

•Flare shows enhanced emission in almost all wavelength, from long to short, including radio, optical, UV, soft X-rays, hard X-rays, and γ-rays

•Flare emissions are caused by thermal plasma heating, and non-thermal particle acceleration

•Heating and particle acceleration are believed to be caused by magnetic reconnection in the corona

•Flares release 1027 - 1032 ergs energy in a few to tens of minutes. (Note: one H-bomb: 10 million TNT = 5.0 X 1023 ergs)

Page 7: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Example in optical Hα

Heating: temperature increase in ChromosphereStructure: Hα ribbons

Page 8: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Example in EUV (~ 195 Å)

TRACE Observation: 2000 July 14 flare

•Heating: temperature increase in corona•Structure

• EUV ribbons• Loop arcade• Filament eruption

Page 9: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Example in soft X-rays (~ 10 Å)

Heating: temperature increase in CoronaStructure: fat X-ray loops

Page 10: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Example in hard X-ray (< 1 Å)

RHESSI in hard X-rays (red contour, 20 Kev, or 0.6 Å) and (blue contour, 100 Kev, or 0.1 Å)•Non-thermal emission: due to energetic electron through Bremsstrahlung (braking) emission mechanism

Page 11: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Example in radio (17 Ghz)

Nobeyama Radioheliograph (17 Ghz, or 1.76 cm) and (34 Ghz, or 0.88 cm)•Non-thermal emission

• due to non-thermal energetic electron and magnetic field• emission mechanism: gyro-synchrotron emission

Page 12: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare Frequency

At solar minimum:1 event/per day

At solar Maximum:10 events/per day

GOES X-ray flare:11696 events From 1996 Jan. To 2001 Dec.

Page 13: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flares: X-ray Classification

Class Intensity

(erg cm-2 s-1)

I (W m-2)

B 10-4 10-7

C 10-3 10-6

M 10-2 10-5

X 10-1 10-4

Page 14: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Hα Classification

Area

(millionth of a solar hemisphere)

Area

(in square degree heliocentric)

Size Important

<100 <2.06 S (Sub-flare)

100---250 2.06—5.15 1

250--600 5.15---12.4 2

600---1200 12.4---24.7 3

>1200 >24.7 4

•Brightness Importance•F: faint•N: Normal •B: Brilliant

•e.g., 3B means covering >12.4 deg2 and exceptionally bright

Page 15: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Temporal Property

• A flare may have three phases:• Preflare phase: e.g., 4 min from 13:50 UT – 13:56 UT• Impulsive phase: e.g., 10 min from 13:56 UT – 14:06 UT• Gradual phase: e.g., many hours after 14:06 UT

Page 16: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Temporal Property (Cont.)

• Pre-flare phase: flare trigger phase leading to the major energy release. It shows slow increase of soft X-ray flux

• Impulsive phase: the flare main energy release phase. It is most evident in hard X-ray, γ-ray emission and radio microwave emission. The soft X-ray flux rises rapidly during this phase

• Gradual phase: no further emission in hard X-ray, and the soft X-ray flux starts to decrease gradually.• Loop arcade (or arch) starts to appear in this phase

Page 17: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Spectrum Property

• The emission spectrum during flare’s impulsive phase

Page 18: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare: Spectrum Property (cont.)• A full flare spectrum may have three components:

1. Exponential distribution in Soft X-ray energy range (e.g., 1 keV to 10 keV): • thermal Bremsstrahlung emission

2. Power-law distribution in hard X-ray energy range (e.g., 10 keV to 100 keV): • non-thermal Bremstrahlung emission• dF(E)/dE = AE–γ Photons cm-2 s-1 keV-1

Where γ is the power-law index

3. Power-law plus spectral line distribution in Gamma-ray energy range (e.g., 100 keV to 100 MeV)• non-thermal Bremstrahlung emission• Nuclear reaction

Page 19: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Bremsstrahlung Spectrum

• Bremsstrahlung emission (German word meaning "braking radiation") • the radiation is produced as the electrons are deflected in

the Coulomb field of the ions.

Bremsstrahlung emission

Page 20: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare Energy Source

•Magnetic energy is slowly-built-up and stored in the corona, and then through a sudden release to produce flares, the so called storage-release model

•Flare is believed to be caused by magnetic reconnection in the corona

•Magnetic reconnection is a process that can rapidly release magnetic energy in the corona

Page 21: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Magnetic Reconnection

•MHD equations

(Aschwanden 6.1.36, P. 247)

•Magnetic field diffusion time τd in the corona τd = 4πσL2/c2 = L2/η

τd the time scale the magnetic field in size L dissipate away,σ electric conductivity, η magnetic diffusivity, L the magnetic field scale size

•In normal coronal condition, τd ~ 1014 s, or 1 million year (assuming L=109 cm, T=106 K, and σ =107T3/2 s-1)

•To reduce τd, reduce L to an extremely thin layer

BcBVtB

)(4

2)(

Page 22: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Magnetic Reconnection: 2-D (cont.)

• quick magnetic energy dissipates at the current sheet (a magnetic neutral sheet) that separates two magnetic regimes, which1. have different directions (opposite directions2. are forced to push together by a continuous converging

motion

• Analytic solutions are obtained by • Sweet-Parker model• Petschek model (Aschwanden book, Chap. 10, p.408-412)

Page 23: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Magnetic Reconnection: 2D (cont.)

Sweet-Parker reconnection

Petschek reconnection

(Aschwanden Book, Fig. 10.2, P411)

Page 24: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Magnetic Reconnection: 3-D (cont.)

(Aschwanden Book, Fig. 10.10, P423)

Page 25: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Magnetic Reconnection: 3-D (cont.)

• Separatrix surface: 2D surface divides oppositely directed magnetic field in 3D volume

• Separator line: 1D intersection lines of two 2D-separatrix surface

• Nullpoint: nullpoint of the intersection of 1D separator lines

• Magnetic reconnection occurs in these locations where current is concentrated and magnetic field is zero

Page 26: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare Model: standard 2-D model

•Aschwanden book. Fig. 10.20, P437

Page 27: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare Model: standard 2-D model (cont.)

• The initial driver of the flare process is a rising flux rope or filament above the neutral line (pre-flare phase)

•At a critical point, the magnetic reconnection at the X-type region below the flux rope sets-in (major flare phase)

•Newly reconnected field lines beneath the reconnection points have an increasingly larger height and wider footpoint separation (post-flare phase)

Page 28: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare dynamic Model

A cartoon model by Gurman

•Particle precipitation

•Thermal conduction

•Chromospheric Evaporation

Page 29: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Flare Dynamic Model (cont.)

•Loop structure of soft X-ray emission•Compact hard X-ray sources appear at two foot-points of soft X-ray loop•Hard X-ray sources appear at top of soft X-ray loops

Page 30: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Coronal Mass Ejection and Filament Eruption

•Both are large scale structural eruption in the corona

•CMEs are observed in the outer corona by coronagraphs (since 1970s)

•Filament Eruption are observed in Hα on the solar disk (since ~1900s)

•CME eruptions are often associated with filament eruption

Page 31: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Filament Eruption

BBSO Hα Mt. Wilson Magnetogram

Page 32: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Filament Eruption (cont.)

•A filament always sits along the magnetic inversion line (magnetic neutral line) that separates regions of different magnetic polarity

•A filament is supported by coronal magnetic field in a supporting configuration

•Magnetic dip at the top of loop arcade (2-D)•Magnetic flux rope (3-D)

•Helical or twisted magnetic structure is seen within filament

Page 33: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Filament Eruption (cont.)

•One of filament models: filament is supported by twisted magnetic flux rope

Page 34: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Filament Eruption (cont.)

Page 36: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Filament Eruption Model

•model of Martens & Kuin

•A unified model of•Filament and•Flare

Page 37: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CMEs

• A CME is a large scale coronal plasma (and magnetic field structure) structure ejected from the Sun, as seen by a coronagraph

• A CME propagates into interplanetary space. Some of them may engulf the earth orbit and cause a series of geo-space activities, such as geomagnetic storms.

• A CME disturbs the solar wind, drives shock in interplanetary space, and produce energetic particles at the shock front.

Page 38: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Coronagraph

• Coronagraph• A telescope equipped with an occulting disk that

blocks out light from the disk of the Sun, in order to observe faint light from the corona

• A coronagraph makes artificial solar eclipse

• The earliest CME observation was made in early 1970s

Page 39: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Coronagraph: LASCO

•C1: 1.1 – 3.0 Rs (E corona) (1996 to 1998 only)•C2: 2.0 – 6.0 Rs (white light) (1996 up to date)•C3: 4.0 – 30.0 Rs (white light) (1996 up to date)

C1 C2 C3•LASCO uses a set of three overlapping coronagraphs to maximum the total effective field of view. A single coronagraph’s field of view is limited by the instrumental dynamic range.

Page 40: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Coronagraph (cont.)

• White light corona has three components:

• K (continuum) corona, caused by scattering of photospheric light of rapidly-moving coronal electrons (so called Thomson scattering); the major component of white-light corona

• F (Fraunhofer corona), caused by scattering of photospheric light off dust in interplanetary space between the orbits of Mercury and Earth

• E (Emission corona), caused by emission of radiation by highly-ionized species in the actual corona, so called forbidden emission lines, e.g., at 5302 Å from Fe XIV (coronal green line)

Page 41: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Coronagraph (cont.)

• K corona: continuum• F corona: continuum plus absorption• E corona: emission lines

Page 42: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Coronagraph (cont.)

• K corona brightness is less than 10-5 that of disk• Space observation is necessary• Special instrumental design to reduce scattering of light

in instrument

Page 43: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Streamer

Several streamers in a typical coronagraph image

Page 44: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Streamer (cont.)

•A streamer is a stable large-scale structure in the white-light corona.

•It has an appearance of extending away from the Sun along the radial direction•It is often associated with active regions and filaments/filament channels underneath.•It overlies the magnetic inversion line in the solar photospheric magnetic fields. •When a CME occurs underneath a streamer, the associated streamer will be blown away•When a CME occurs nearby a streamer, the streamer may be disturbed, but not necessarily disrupted.

Page 45: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME: transient phenomenon (example)

A LASCO C2 movie, showing multiple CMEs

Page 46: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME Property: Measurement

H (height, Rs)

PA (position angle)

AW (angular width)

M (mass)

Page 47: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME Property: velocity

•Velocity is derived from a series of CME H-T (height-time) measurement

•A CME usually has a near-constant speed in the outer corona (e.g, > 2.0 Rs in C2/C3 field)

•Note: such measured velocity is the projected velocity on the plane of the sky; it is not the real velocity in the 3-D space.

Page 48: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME Property: velocity distribution

6300 LASCO CMEs from 1996 to 2002

•CME velocity50 km/s to 3000 km/s

•Average vel.: 400 km/s

•Peak vel.: 300 km/s

•Median vel.: 350 km/s

Page 49: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME Property: size

AW = 80 degree AW = 360 degree, halo CME

Page 50: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME Property: size

•Broad distribution of CME apparent angular width

•Average width 50 degree

•A number of halo CMEs (AW=360 degree), or partial halo CMEs (AW > 120 degree)

•Halo CMEs are those likely to impact the Earth orbit

Page 51: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME Property: mass

•CME mass distribution from 1013 to 1016 gram

•Average CME mass about 1015 gram

Based on2449 LASCO CMEsFrom 1996 to 2000

Page 52: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME Morphology

Page 53: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME morphology (cont)

• Three part CME structure1. A bright frontal loop (or leading edge)

• Pile-up of surrounding plasma in the front2. A dark cavity (surrounded by the frontal loop)

• possibly expanding flux rope or filament channel3. A bright core (within the cavity)

• Composed of densely filament remnant material

Page 54: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

kinematic Evolution of a CME

• A CME is strongly accelerated in the inner corona (<2 Rs) (Zhang et al., 2001, 2004)

• A CME maintains a more or less constant speed when it travels in the outer corona (>2 Rs)

Page 55: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

Geo-effective CMEs: halo CMEs

• Whether a CME is able to intercept the Earth depends on its propagation direction in the heliosphere.

• A halo CME (360 degree of angular width) is likely to have a component moving along the Sun-Earth connection line

• A halo is a projection effect; it happens when a CME is initiated close to the disk center and thus moves along the Sun-Earth connection line.

• Therefore, a halo CME is possibly geo-effective.

2000/07/14

C2 EIT

Page 56: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME modelsA model shall include many observational elements

•CME• front• cavity• core

•Flare•X-ray loop•EUV loop arcade•Hα flare ribbon

•Magnetic reconnection •Current sheet•Reconnection inflow

•Some Others•filament eruption•coronal dimming•timing relation•Energetic relation

Page 57: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME models (cont.)

Lin’s CME eruption model• MHD analytic solution•Animation

Page 58: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME models (cont.)

Aschwanden book:Fig. 17.3, P710:

Numeric SimulationBy Amari et al

Page 59: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

CME models (cont.)

Antiocs’s CME eruption model•MHD numeric solution •Multi-polar•So-called break-out model

Page 60: CSI 769/ASTR 769 Topics in Space Weather Fall 2005 Lecture 03 Sep. 13, 2005 Solar Eruptions: Flares and Coronal Mass Ejections Aschwanden, “Physics of

The End