HR: 16:15h
AN: SH54B-04 [Abstracts]
TI: In situ observation of filament plasma and their magnetic structure
AU: * Zurbuchen, T H
EM: thomasz@umich.edu
AF: Department of AO&SS, University of Michigan
2455 Hayward St, Ann Arbor, MI 48109 United States
AU: Raines, J
EM: jraines@umich.edu
AF: Department of AO&SS, University of Michigan
2455 Hayward St, Ann Arbor, MI 48109 United States
AU: Lynch, B
EM: lynchb@umich.edu
AF: Department of AO&SS, University of Michigan
2455 Hayward St, Ann Arbor, MI 48109 United States
AU: Lepri, S
EM: slepri@umich.edu
AF: Department of AO&SS, University of Michigan
2455 Hayward St, Ann Arbor, MI 48109 United States
AU: Gloeckler, G
EM: gg10@umail.umd.edu
AF: Department of AO&SS, University of Michigan
2455 Hayward St, Ann Arbor, MI 48109 United States
AU: Gloeckler, G
EM: gg10@umail.umd.edu
AF: Department of Physics, University of Maryland, College Park, MD 20742 United States
AU: Fisk, L
EM: lafisk@umich.edu
AF: Department of AO&SS, University of Michigan
2455 Hayward St, Ann Arbor, MI 48109 United States
AB:
Many CMEs, when observed during their expansion in the corona, are associated with a three-part structure: A bright core
associated with prominence plasma, a dark area or cavity, that is bounded by a bright rim, presumably associated with the
dynamic interactions of CMEs with their plasma environment. Many Interplanetary CMEs (ICMEs) only have two key parts: A
magnetically dominated inner part, generally associated with the low density volume appearing dark in the corona, and the
interaction sheath, presumably associated with the interaction of magnetic clouds in the corona. The vast majority of ICME do not have recognizable filament plasma.
There are a few observations of ICMEs with singly charged He contributions that are generally associated with filaments.
However, there are two model scenarios for producing such low ionic charge states. First, they can be achieved through
filament-like material that never heats up during the eruption. Second, they can result from a rapid freeze-in process at
high density in the corona. We discuss in situ observations of ICMEs that are characterized by unusually cool material and
the ionic composition of all observable constituents that allow us to distinguish between these models. We discuss these data and interpret them in the context of CME models and the evolution of CMEs in the inner corona. We will also discuss the
relation of the filament material to the magnetically dominated structures, such as flux ropes.
DE: 2164 Solar wind plasma
DE: 7524 Magnetic fields
DE: 7531 Prominence eruptions
SC: SPA-Solar and Heliospheric Physics [SH]
MN: 2005 Joint Assembly