2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive...

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2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J. G. Luhmann S. K. Antiochos, C. R. DeVore
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Transcript of 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive...

Page 1: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

2007 PROM WORKSHOPSpace Sciences Lab / UC-Berkeley

Sheared-Field Prominences and the Eruptive Implications of Magnetic

Topology

B. J. Lynch, Y. Li, J. G. LuhmannS. K. Antiochos, C. R. DeVore

Page 2: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Two Basic CME Source Region Topologies

approximately

[Y. Li, 2006]

[Y. Li, 2006]

approximately

bipo

lar

mul

tipo

lar

Page 3: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Emo : “Maximally Open” ( 0% blue-red reconnection )

Emc : “Maximally Closed”( 100% blue-red reconnection )

Topology Determines Open State(s)bi

pola

rm

ulti

pola

r

only one Open State possibility

[DeVore et al., 2005]

Page 4: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

B2

[DeVore et al., 2005]

[MacNeice et al., 2004]

(Br2+B

2)K.E.

0% rxn

100% rxn

Energy Evolution of MultipolarConfiguration in 2.5D

In MHD treatments of multipolar topologies, you can approach the no-reconnection limit before it “switches on”

Page 5: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Magnetic Neutral Lines

3D Null Point

Bipolar Multipolar

Magnetic Topologies in 3D

Magnetic Neutral Line

Page 6: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Bipolar Multipolar

Surface Field Evolution

Page 7: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Radial Velocity Evolution (=0)

Bipolar Multipolar

Page 8: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Magnetic Fieldline Evolution

Bipolar Multipolar

t = 15000 s

Page 9: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Flare reconnection starts

Magnetic + Kinetic Energy Evolution

Bipolar: EM(0) = 4.117e+31 ergsMultipolar: EM(0) = 2.566e+31 ergs

Initial (Potential) Magnetic Energies

EM=EM(t)-EM(0)

Notice the magnetic energy signature of the Br diffusion

EDIFF ~ 3.90e+31 ergs !!

Moderately fast breakout eruption (~500 km/s), but the rapid conversion from EM EK not super impressive

BUT, the Bipolar case doesn’t show any sign of eruption!

Page 10: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Summary & Current/Future Work

Bipolar Arcades Don’t Erupt Without Something Else Happening !!!

• Aly-Sturrock holds up in 3D!• Breakout works in 3D and probably for the reasons we think…• Theorists & modelers may still be relevant!

• Next simulation—• Get rid of that inner-boundary Br diffusion!• Slower driving, “cleaner” magnetic, kinetic energy profiles

(so far, so good… )

t = 5000 s t = 7500 s t = 10000 s

Page 11: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

Sheared Field Prominence Structure

Three perspectives of the non-eruptive Bipolar fieldlines at t=15,000 seconds

Essentially the spherical version of sheared-arcade prominence model…[DeVore & Antiochos, 2000 and others]

Page 12: 2007 PROM WORKSHOP Space Sciences Lab / UC-Berkeley Sheared-Field Prominences and the Eruptive Implications of Magnetic Topology B. J. Lynch, Y. Li, J.

3D Erupting Fieldlines3D Erupting Fieldlines

And because we can’t let the data folks have all the fun…