Kinetic models of the solar wind
A kinetic model of the solar wind with Kappa distributions in the
corona
Maksimovic, M., V. Pierrard and J. Lemaire, Astronomy
and Astrophysics, 324, 725-734, 1997.
A kinetic model of the solar wind based on Kappa velocity
distribution functions for the electrons and protons escaping out
of the corona is presented. The high velocity particles forming
the tail of these distribution functions have been introduced in
the pioneering work of Scudder (1992a,b) to explain the high temperature
of the coronal plasma. The first results obtained with this new
kinetic model of the solar wind are very encouraging, indeed they
fit better many major features observed in the solar wind than earlier
models: e.g. the large bulk velocities observed in high speed streams
emitted out from the coronal regions where the plasma temperature
is smaller, and the low speed solar wind originating in the hotter
equatorial regions of the solar corona. This new kinetic model is
also able to predict the high speed solar wind streams without additional
heating of the outer region of the corona, as it is needed in hydrodynamic
models to achieve the same solar wind speed.
Ulysses electron distributions fitted with Kappa functions
M. Maksimovic, V. Pierrard and P. Riley Geophys Res.
Let., 24, 9, 1151-1154, 1997.
We fit Kappa functions to 16,000 velocity distribution
functions measured in the solar wind by the electron plasma instrument
on board Ulysses. Statistically, the electron distributions are
observed to have important high velocity tails in the fast solar
wind but are closer to a Maxwellian in the slow wind. We also discuss
how this result could support a recent kinetic model of the solar
wind proposed by Maksimovic, Pierrard and Lemaire [1997].
Electron velocity distribution functions from the solar wind to
the corona
V. Pierrard, M. Maksimovic, and J. Lemaire Journ.
Geophys. Res., 104, 17021-17032, 1999.
Typical electron velocity distribution functions observed
at 1 AU from the Sun by the instrument 3DP aboard of WIND are used
as boundary conditions to determine the electron velocity distribution
function at 4 solar radii in the corona. The velocity distribution
functions (VDF) at low altitude are obtained by solving the Fokker-Planck
equation, using two different sets of boundary conditions. The first
set typically corresponds to a VDF observed in a low speed solar
wind flow (i.e.\ characterized by "core" and "halo" electrons);
the second one corresponds to high speed solar wind (i.e. characterized
by "core", "halo" and "strahl" populations). We use the observed
electron VDFs as test particles which are submitted to external
forces and Coulomb collisions with a background plasma. Closer to
the Sun, the relative density of the core electrons is found to
increase compared to the density of the halo population. Nevertheless,
we find that in order to match the observed distributions at 1 AU,
suprathermal tails have to be present in the VDF of the test electrons
at low altitudes in the corona.
Author:
V. Pierrard Curator: V.
Pierrard V.Pierrard@bira-iasb.oma.be