Rl. Moore et al., On heating the sun's corona by magnetic explosions: Feasibility in active regions and prospects for quiet regions and coronal holes, ASTROPHYS J, 526(1), 1999, pp. 505-522
We build a case for the persistent strong coronal heating in active regions
and the pervasive quasisteady heating of the corona in quiet regions and c
oronal holes being driven in basically the same way as the intense transien
t heating in solar hares: by explosions of sheared magnetic fields in the c
ores of initially closed bipoles.
We begin by summarizing the observational case for exploding sheared core f
ields being the drivers of a wide variety of flare events, with and without
coronal mass ejections. We conclude that the arrangement of an event's har
e heating, whether there is a coronal mass ejection, and the time and place
of the ejection relative to the flare heating are all largely determined b
y four elements of the form and action of the magnetic field: (1) the arran
gement of the impacted, interacting bipoles participating in the event, (2)
which of these bipoles are active (have sheared core fields that explode)
and which are passive (are heated by injection from impacted active bipoles
), (3) which core held explodes first, and (4) which core-field explosions
are confined within the closed field of their bipoles and which ejectively
open their bipoles.
We then apply this magnetic-configuration framework for flare heating to th
e strong coronal heating observed by the Yohkoh Soft X-ray Telescope in an
active region with strongly sheared core fields observed by the Marshall Sp
ace Flight Center vector magnetograph. All of the strong coronal heating is
in continually microflaring sheared core fields or in extended loops roote
d against these active core fields. Thus, the strong heating occurs in fiel
d configurations consistent with the heating being driven by frequent core-
held explosions that are smaller than but similar to those in confined flar
es and flaring arches. From analysis of the thermal and magnetic energetics
of two selected core-field microflares and a bright extended loop, we find
that (1) it is energetically feasible for the sheared core fields to drive
all of the coronal heating in the active region via a staccato of magnetic
microexplosions, (2) the microflares at the feet of the extended loop beha
ve as the flares at the feet of flaring arches in that more coronal heating
is driven within the active bipole than in the extended loop, (3) the fill
ing factor of the X-ray plasma in the core field microflares and in the ext
ended loop is similar to 0.1, and (4) to release enough magnetic energy for
a typical microflare (10(27)-10(28) ergs), a microflaring strand of sheare
d core field need expand and/or untwist by only a few percent at most.
Finally, we point out that (1) the field configurations for strong coronal
heating in our example active region (i.e., neutral-line core fields, many
embedded in the feet of extended loops) are present in abundance in the mag
netic network in quiet regions and coronal holes, and (2) it is known that
many network bipoles do microflare and that many produce detectable coronal
heating. We therefore propose that exploding sheared core fields are the d
rivers of most of the heating and dynamics of the solar atmosphere, ranging
from the largest and most powerful coronal mass ejections and flares, to t
he vigorous microflaring and coronal heating in active regions, to the mult
itude of fine-scale explosive events in the magnetic network, which drive m
icroflares, spicules, global coronal heating, and, consequently, the solar
wind.