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temperature at that height in coronal holes is expected to be less than 106 K. Similarly, in equatorial streamers, v1/e
along the LOS for protons and O5+ become equal at 4.7 RSun
at values corresponding to 1.3 x 106K (protons) and
2.1 x 107 K (O5+). In other

words, not only are the kinetic temperatures larger for the higher mass particles, which is contrary to most earlier theoretical

models, but also the velocities are extremely large.

The higher O5+ velocities compared to protons in polar coronal holes can not be explained by transverse wave motions caused

by MHD wave propagation through the corona. They are, however, consistent with theoretical models in which charged par-

ticles are accelerated about the coronal magnetic field through ion cyclotron resonant acceleration by relatively high frequency

MHD waves, which are assumed to exist. Further evidence for the ion cyclotron resonance process in the corona has been

obtained by deriving the O 5+ velocity distribution along the radial direction from the intensity ratio of the O VI 1032 and 1037

Å lines, which are formed by a combination of collisional excitation and resonant scattering. The radial velocities, which are

expected to be parallel to the magnetic field lines in polar coronal holes, are at least a factor of 6 smaller than LOS values, which

are expected to be approximately perpendicular to the magnetic field in polar coronal holes. The ion cyclotron resonance

process appears to operate in both coronal holes and equatorial streamers. Thermalizing collisions may mask the evidence for

the process in the highest density regions. Work is continuing to determine to what degree coronal heating can be explained by

the ion cyclotron resonance process, and to search for independent evidence for the existence of the required high frequency

MHD waves.

Large-Scale Coronal Structure and Events

The vastly improved dynamic range of LASCO compared to previous coronagraphs and its 30 R Sun field of view are revolution-

izing our concept of the solar corona. Presented in movie form the LASCO data have, for the first time, revealed the small scale

jets, eruptions, and reconfigurations associated with both the gradual and disruptive evolution of coronal structures. At low

altitudes, beneath the helmet streamer structure, the corona consists of large-scale magnetic loops associated with the small

active regions present at this phase of the solar cycle. LASCO movies have shown that these loops are continually expanding

outward. This continual expansion appears to provide sufficient mass and energy to completely regenerate the equatorial

current sheet in a short period of time and to ultimately disrupt the streamer as a coronal mass ejection.
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gested that the corona evolved on time scales of days, with disruptions by large-scale CME's. LASCO observations show that

coronal mass ejections occur at a rate that is apparently more frequent than during previous solar minima. The CME's can be

large and as bright as those seen in the past, but in addition there are many smaller, less massive events. These observations

show that coronal structures evolve continally in a manner consistent with the frequent generation of CME's with a large range

of sizes. UVCS spectroscopic observations of CME's have shown bulk Doppler velocitiesof up to 200 km s - 1.

Many of the CME's observed with LASCO indicate that a large portion of the solar corona must be involved in the CME

process. These 'global CME's' are accompanied by small but obvious ejecta on the opposite limb. How the corona organizes

itself to generate such a global phenomenon is a major new problem for SOHO to attack.

Sources of the Solar Wind

It is well known that the large scale magnetic structure of the Sun determines the overall structure of the corona. Compact active

regions give rise to compact loops, which are imbedded in larger helmet-shaped regions, which are capped by long streamers.

The low-speed solar wind originates from these streamer belts and perhaps from between the streamers. Much larger diffuse

unipolar regions can generate open field regions in the corona--coronal holes. These open regions give rise to the high speed

solar wind. While the locations of these wind components are understood in a global sense, only now is SOHO revealing the

mechanisms that power the wind and the specific locations of the acceleration regions.

Slow Speed Wind. Time-lapse sequences of coronal images obtained with LASCO have yielded important clues on the origin

and acceleration of the slow speed wind. Because of LASCO's sensitivity, dynamic range, and field of view, bits and fragments

of material can be observed that appear to be torn off the tops of coronal streamers and carried passively outward like "leaves in

the terrestrial wind." The speed of the typical fragment doubles from 150 km s - 1 at 5 R Sun to 300 km s - 1 at 25 R Sun. By tracking

the outward movement and assuming that the fragments are tracers of a flow field, a constant acceleration of about 4 m s - 2

through the coronagraph's 2-30 R Sun field of view is inferred. For a thermally driven wind, this implies that the coronal tempera-

ture does not fall off rapidly with radial distance as it would for an adiabatic expansion, but remains constant at about 1.1 MK

out to 10-15 RSun and that the sonic point is near 5 RSun .
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