1 / 11

CME Propagation

CSI 769 / ASTR 769 Lect. 11, April 10 Spring 2008. CME Propagation. CME Flux Rope Model. Lepping, R.P., Jones, J.A., Burlaga. “Magnetic Field Structure of Interplanetary Magnetic Clouds at 1 AU” JGR, Vol. 95, No. A8, 11957-11965, 1990. CME MSOE Model.

kalei
Download Presentation

CME Propagation

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. CSI 769 / ASTR 769 Lect. 11, April 10 Spring 2008 CME Propagation

  2. CME Flux Rope Model Lepping, R.P., Jones, J.A., Burlaga. “Magnetic Field Structure of Interplanetary Magnetic Clouds at 1 AU” JGR, Vol. 95, No. A8, 11957-11965, 1990

  3. CME MSOE Model Siscoe, G.L., Crooker, N.U., Elliott, H.A., “Initial-Condition Influences on CME Expansion and Propagation” Solar Physics, Vol. 239, 293-316, DOI: 10.1007/s11207-006-0302-3, 2006 MSOE: Melon-Seed-Overpressure-Expansion Model

  4. Interplanetary CME (ICME) • CME propagates into the interplanetary space, plowing through the ambient solar wind • The magnetic structure of ICME at 1 AU is similar to that in its solar origin, which is highly helical (called flux rope) • At 1 AU, it is called magnetic cloud • highly organized magnetic field is observed, e.g., smooth rotation • Large scale, crossing the Earth for ~ 24 hours Magnetic Cloud

  5. ICME Identification Dst B/Bz Vel Np Tp Texp β Sun 2004/07/27 storm (-182 nT) Shock Front: discontinuity • ICME (ejecta): • B enhance • Bz rotation • Low Plasma β • Low Tp • High QFe • ----- SH (Shock Sheath) Solar Sources

  6. Fast and Slow Wind Solar Wind: Bimodal Fast wind originates from coronal hole, Slow wind originates from regions close to streamer belts or heliospheric current sheet SW heliographic latitudinal Distribution (Ulysses observation)

  7. Corotating Interaction Region (CIR) • When a low latitude coronal hole appears (across the heliographic equator), fast wind exists in the ecliptic plane.

  8. Corotating Interaction Region (CIR) • The jetline of fast wind is less curved than that of slow wind • Fast streams “catching up” with slow streams, compressing the preceding stream and produce a high pressure region. • The interaction region is at the leading edge of the fast stream • Since low-latitude coronal holes can live over several solar rotations, this structure can recur several times • This is commonly called “corotating interaction region” or CIR • A pair of forward and reverse shocks forms

  9. CIR Corotating Interaction Region: Caused by the interaction of fast SW originated from coronal hole with preceding slow SW CIR/SI

  10. IMF

  11. The End

More Related