A NEW CRITERION FOR BAR-FORMING INSTABILITY IN RAPIDLY ROTATING GASEOUS AND STELLAR-SYSTEMS .1. AXISYMMETRICAL FORM

We analyze previous results on the stability of uniformly and differentially rotating, self-gravitating, gaseous and stellar, axisymmetric systems to derive a new stability criterion for the appearance of toroidal, m = 2 intermediate or I-modes and bar modes. In the process, we demonstrate that the bar modes in stellar systems and the m = 2 I-modes in gaseous systems have many common physical characteristics and only one substantial difference: because of the anisotropy of the stress tenser, dynamical instability sets in at fewer rotation in stellar systems. This difference is reflected also in the new stability criterion. The new stability parameter alpha = T-J/\W\ is formulated first for uniformly rotating systems and is based on the angular momentum content rather than on the energy content of a system. (T-J = L Omega(J)/2; L is the total angular momentum; Omega(J) is the Jeans frequency introduced by self-gravity; and W is the total gravitational potential energy.) For stability of stellar systems alpha less than or equal to 0.254-0.258 while alpha less than or equal to 0.341-0.354 for stability of gaseous systems. For uniform rotation, one can write alpha = (ft/2)(1/2), where t = T/\W\, T is the total kinetic energy due to rotation, and f is a function characteristic of the topology/connectedness and the geometric shape of a system. Equivalently, alpha = t/chi, where chi = Omega/Omega(J) and Omega is the rotation frequency. Using these forms, alpha can be extended to and calculated for a variety of differentially rotating, gaseous and stellar, axisymmetric disk and spheroidal models whose equilibrium structures and stability characteristics are known. In this paper, we also estimate a for gaseous toroidal models and for stellar disk systems embedded in an inert or responsive ''halo.'' We find that the new stability criterion holds equally well for all these previously published axisymmetric models.