K. Otmianowskamazur et M. Chiba, NUMERICAL-SIMULATION OF LARGE-SCALE MAGNETIC-FIELD EVOLUTION IN SPIRAL GALAXIES, Astronomy and astrophysics, 301(1), 1995, pp. 41-54
The evolution of large-scale magnetic fields in disk galaxies is inves
tigated numerically. The gasdynamical simulations in a disk perturbed
by spiral or bar potential are incorporated into the kinematic calcula
tions of induction equations to elucidate the effects of non-axisymmet
ric disk structure on magnetic fields. The effects of interstellar tur
bulence are given as the turbulent diffusion of magnetic fields. The u
sually adopted dynamo mechanism of alpha-effect is not considered in o
ur computations, because it is not obvious about the actual existence
of the effect in a galaxy. Our principal concern is to clear how obser
vationally and theoretically well-established gas flow affects the mag
netic-field structure and evolution, without putting a lot of artifici
al parameters in the model. We have found that the density-wave stream
ing motion of gas has a significant influence on the distribution of m
agnetic fields: the lines of force are well aligned with spiral arms d
ue to the compressional and additional shearing flow of gas in these r
egions. In the inter-arm regions, the field lines have the finite angl
es with respect to the imposed arms, because the gaseous streamlines i
nduced by spiral arms deviate from the orientation of spiral arms them
selves. These properties of magnetic-field orientation across the arm
are well in agreement with the results of radio continuum observations
. All simulation models have resulted in the eventual decay of magneti
c energy due to the strong turbulent diffusion. We have also explored
the azimuthally periodic function for the coefficient of turbulent dif
fusion with the maximum in spiral-arm regions. This is anticipated fro
m the enhancement of turbulence by young OB stars and supernovae. This
effect of non-uniform dissipation gives rise to the modulation of mag
netic-field structure and its time evolution. In particular, the dissi
pation rate of magnetic fields can be much smaller than the usually as
sumed rate of similar to 1/10(8) yr(-1).