TILTING OF A DISK OF SELF-GRAVITATING RINGS

Authors
Citation
Rve. Lovelace, TILTING OF A DISK OF SELF-GRAVITATING RINGS, Astronomy and astrophysics (Berlin), 338(3), 1998, pp. 819-839
Citations number
27
Categorie Soggetti
Astronomy & Astrophysics
ISSN journal
00046361
Volume
338
Issue
3
Year of publication
1998
Pages
819 - 839
Database
ISI
SICI code
0004-6361(1998)338:3<819:TOADOS>2.0.ZU;2-O
Abstract
The present work represents an attempt to understand the 'rules of beh avior' of observed warps in the HI disks of spiral galaxies found by B riggs (1990). In contrast with most earlier theoretical work, the pres ent study investigates different initial value problems of a warped di sk in an oblate (or prolate) halo potential, and it represents the dis k warp in terms of N independently tilted, self-gravitating, concentri c rings. This representation gives new insight into the disk warping. The phenomenon of phase-locking of the lines-of-nodes of nearby rings due to self-gravity is demonstrated. We consider the influence of dyna mical friction due to ring motion through the halo matter as well as f riction between gaseous rings with different vertical motions due to t urbulent viscosity. We first consider the dynamics of one, two, and th ree tilted rings of different radii in a halo potential. We go on to d evelop dynamical equations for N-rings which are most simply expressed in terms of the complex tilt angles Theta(j) = theta(j)exp(-i phi(j)) , where theta(j) is the actual tilt angle and phi(j) the line-of-nodes angle for the j(th) ring (j = 1..N). Relatively small values of N (le ss than or similar to 10(2)) are sufficient to describe the warp evolu tion during the age of a galaxy during which time discrete modes are n ot important. The equations for Theta(j) are solved numerically for fo ur different types of initial conditions: (1) warp excitation by a pas sing satellite, (2) excitation by a sinking compact minor satellite, ( 3) warp evolution due to a tilted halo potential, and (4) warp evoluti on resulting from an initially tilted disk plane. The nature of the wa rps is most clearly shown by the polar plots of theta(j) versus phi(j) .