authors: f. rozpedek , s . r. brannon, d. w. longcope
DESCRIPTION
The effects of canopy expansion on chromospheric evaporation driven by thermal conduction fronts. Authors: F. Rozpedek , S . R. Brannon, D. W. Longcope. Credit: M. Aschwanden et al. ( LMSAL ), TRACE , NASA. Flare loop dynamics. Reconnection frees loop to contract. RD accels plasma. - PowerPoint PPT PresentationTRANSCRIPT
The effects of canopy expansion on chromospheric evaporation driven by thermal
conduction fronts
Authors: F. Rozpedek, S. R. Brannon, D. W. Longcope
Credit: M. Aschwanden et al. (LMSAL), TRACE, NASA
RD RDGDSGDS
RD accels plasma
GDS heats plasma to flare temp. @
loop top
Simulationregion
Chromosphere
Reconnection frees loop to
contract
~90% free mag. energy => bulk plasma motion(Longcope et al. 2009)
Flare loop dynamics
1-D “shocktube” model
•Model details:
•Static non-uniform grid:
• <1 km (chromosphere), ~10 km (corona), scales up in TR
•Include viscosity & Spitzer conductivity
•Neglect gravity & explicit radiative effects
•Simplified model atmosphere: temp. grad. @ const.
pressure
•Classical piston shock (tanh func. w/ Rankine-
Hugoniot)
Mp
Ms
ChromosphereT=0.01
CoronaT=1
Uniform pressure in TR
Trans. Reg.(TR)
GDS
Post-shockFluidinput
Model loop atmosphereChromosphere TR Corona
Time Evolution for the uniform tube
TCF
Time Evolution for the uniform tube
TCF
Time Evolution for the uniform tube
E
C
TCF
Time Evolution for the uniform tube
E
C
TCFC
E
Time Evolution for the uniform tubeE
C
TCF
CE
A
CB
TR ??
Question:Is there some observational quantity that would enable us to determine where the nozzle is located relative to the Transition Region?
The canopy expansion
Varying Area Profile
Nozzle below the TRNozzle at the centre
of the TR Nozzle above the TR
The area profile has a form of a piecewise linear function.
ThermalConduction
Front
ThermalConduction
Front
ThermalConduction
Front
Transsonic points(lower) (upper)
Transsonic points (lower) (upper)
Thank You