M. Bzowski et al., VARIATION OF BULK VELOCITY AND TEMPERATURE ANISOTROPY OF NEUTRAL HELIOSPHERIC HYDROGEN DURING THE SOLAR-CYCLE, Astronomy and astrophysics, 326(1), 1997, pp. 396-411
Using a time-dependent kinetic approach the density, bulk velocity vec
tor, and temperature tensor of interstellar hydrogen in the inner Sola
r System in several phases of solar cycle were computed. Model solar c
ycle time-profiles of hydrogen ionisation rate and Lyman-cr radiation
pressure were used, solar latiudinal effects and filtration at the hel
iospheric interface were neglected. It was concluded that due to the j
oint action of solar ionisation and radiation pressure the bulk veloci
ty of the gas is strongly variable during solar cycle and, within 15-3
0 AU from the Sun, it significantly changes with the heliocentric dist
ance both in magnituide and direction. The changes typically are about
15 km/s and exceed the thermal spread of the gas. The temperature is
strongly anisotropic; the anisotropy is strongly variable in time and
it fades off with the heliocentric distance. The projections of temper
ature tensor on various lines can change from 5 000 to 11 000 K upwind
and from similar to 12 000 to 45 000 K downwind at 1 AU and from 6 00
0 to 8 000 K upwind and from 8 000 to 15 000 K downwind at 10 AU. For
optical observations an important quantity is the radial temperature.
For lines of sight directed radially away from the Sun the change of r
adial temperature along the sightline is strongest during solar minimu
m and it is equal to about 3 000 K in the upwind direction and to abou
t 5 000 K in the downwind direction. The smallest change occurs during
solar maximum. The upwind-to-downwind ratio of intensity of backscatt
ered radiation varies during the solar cycle by about 20% around the m
ean value. A brief discussion of theoretical spectra of interplanetary
lines is provided. The main conclusion is that for observations carri
ed out from 1 AU the Doppler shift of interplanetary lines corresponds
to the bulk speed ''in infinity'' for the lines of sight directed dow
nwind; for the lines of sight directed upwind the Doppler shift corres
ponds to the bulk speed increased by about 25% in comparison with the
bulk speed ''in infinity'' except solar maximum epoch, when the increa
se is only 1 to 2 km/s. The width of interplanetary lines returns the
temperature of the gas ''in infinity'' only for the lines of sight dir
ected upwind; for the lines of sight directed crosswind and downwind t
he line width returns temperatures higher by about 3 000 IC and no sim
ple seasonal correlation can be observed.