RECONNECTION AND FIELD LINE SHRINKAGE IN SOLAR-FLARES

Citation
Tg. Forbes et Lw. Acton, RECONNECTION AND FIELD LINE SHRINKAGE IN SOLAR-FLARES, The Astrophysical journal, 459(1), 1996, pp. 330
Citations number
39
Categorie Soggetti
Astronomy & Astrophysics
Journal title
ISSN journal
0004637X
Volume
459
Issue
1
Year of publication
1996
Part
1
Database
ISI
SICI code
0004-637X(1996)459:1<330:RAFLSI>2.0.ZU;2-9
Abstract
We use images of flare loops taken by the Soft X-ray Telescope (SXT) o n Yohkoh to estimate the decrease in height that open field lines unde rgo after they have reconnected to form closed loops. Following previo us practice, we refer to this decrease as field line shrinkage and ass ume that intensity structures trace out the field lines. For this stud y, we examine two long-duration events near the limb which have flare loops that continually grow with time. The shrinkage is determined by comparing the height of a field line when it lies at the outermost edg e of the flare loop system with the height it has later on when it lie s at the innermost edge. We find that the field lines shrink by about 20% of their initial height in one flare and by about 32% in the other . These values are within 5% of the shrinkage predicted by a simple mo del of the reconnecting field which assumes that the field is potentia l everywhere except for a current sheet extending upward from the top of the loops. Numerical integration of the model density along the lin e of sight implies that most of the discrepancy between the observatio ns and the theory is due to projection effects which occur when an arc ade of loops is viewed at an arbitrary angle. Both flares have bright regions at the top of the loops, but in one flare the lower part of th e region is cooler and denser than the rest of the loop, while in the other flare it is not. Consideration of the mapping of the bright regi ons to the footpoint of the loops implies that the cool region is form ed by a thermal instability downstream of a reconnection outflow in th e uppermost part of the loop. The absence of a cool, dense region in t he other flare may be caused by the fact that it is a very weak event with temperatures and densities too low to trigger a thermal instabili ty.