This work studies the hydrodynamics of self-gravitating, compressible, isot
hermal fluids. We show that the hydrodynamic-evolution equations are scale
covariant in the absence of viscosity. Then, we study the evolution of the
time-dependent fluctuations around singular and regular isothermal spheres.
We linearize the fluid equations around such stationary solutions and deve
lop a method based on the Laplace transform to analyze their dynamical stab
ility. We find that the system is stable below a critical size (X similar t
o9.0 in dimensionless variables) and unstable above; this criterion is the
same as the one found for the thermodynamic stability in the canonical ense
mble and it is associated with a center-to-border density ratio of 32.1. We
prove that the value of this critical size is independent of the Reynolds
number of the system. Furthermore, we give a detailed description of the se
ries of successive dynamic instabilities that appear at larger and larger s
izes following the geometric progression X(n)similar to 10.7(n), n=1,2,....
Then, we search for exact solutions of the hydrodynamic equations without
viscosity, we provide analytic and numerical axisymmetric soliton-type solu
tions. The stability of exact solutions corresponding to a collapsing filam
ent is studied by computing linear fluctuations. Radial fluctuations growin
g faster than the background are found for all sizes of the system. However
, a critical size (X similar to4.5) appears, separating a weakly from a str
ongly unstable regime.