ULYSSES FIELD AND PLASMA OBSERVATIONS OF MAGNETIC HOLES IN THE SOLAR-WIND AND THEIR RELATION TO MIRROR-MODE STRUCTURES

Citation
D. Winterhalter et al., ULYSSES FIELD AND PLASMA OBSERVATIONS OF MAGNETIC HOLES IN THE SOLAR-WIND AND THEIR RELATION TO MIRROR-MODE STRUCTURES, J GEO R-S P, 99(A12), 1994, pp. 23371-23381
Citations number
36
Categorie Soggetti
Geosciences, Interdisciplinary","Astronomy & Astrophysics","Metereology & Atmospheric Sciences
Journal title
JOURNAL OF GEOPHYSICAL RESEARCH-SPACE PHYSICS
ISSN journal
21699380 → ACNP
Volume
99
Issue
A12
Year of publication
1994
Pages
23371 - 23381
Database
ISI
SICI code
2169-9380(1994)99:A12<23371:UFAPOO>2.0.ZU;2-Y
Abstract
The term ''magnetic hole'' has been used to denote isolated intervals when the magnitude of the interplanetary magnetic field drops to a few tenths, or less, of its ambient value for a time that corresponds to a linear dimension of tens to a few hundreds of proton gyro-radii. Dat a obtained by the Ulysses magnetometer and solar wind analyzer have be en combined to study the properties of such magnetic holes in the sola r wind between 1 AU and 5.4 AU and to 23 degrees south latitude. In or der to avoid confusion with decreases in field strength at interplanet ary discontinuities, the study has focused on linear holes across whic h the field direction changed by less than 5 degrees. The holes occurr ed preferentially, but not without exception, in the interaction regio ns on the leading edges of highspeed solar wind streams. Although the plasma surrounding the holes was generally stable against the mirror i nstability, there are indications that the holes may have been remnant s of mirror-mode structures created upstream of the points of observat ion. Those indications include the following: (1) For the few holes fo r which proton or alpha-particle pressure could be measured inside the hole, the ion thermal pressure was always greater than in the plasma adjacent to the holes. (2) The plasma surrounding many of the holes wa s marginally table for the mirror mode, while the plasma envitonmen?t of all the holes was significantly closer to mirror instability than w as the average salar wind. (3) The plasma containing trains of closely spaced holes was closer to mirror instability tl;an was the plasma co ntaining isolated holes. (4) The near-hole plasma had much higher ion beta (ratio of thermal to magnetic pressure) than did the average sola r wind. (5) Near the holes, T-perpendicular to/T-II tended tb be eithe r >1 or larger than in the average wind. (6) The proton and alpha-part icle distribution function's measured inside the holes occasionally ex hibited the flattened phase-space-density contours in nu(perpendicular to)-nu(II) space found in some numerical simulations of the mirror in stability.