“…Consider a viscous incompressible fluid with a density e and a kinematic viscosity v in a closed domain D with a rigid boundary r; characteristic length of D is equal to d. The governing equations in the dimensionless variables can be written in the following form (3) be an external force. Assume that V = V,(z; R) 7 1., =Po@; R) (4) is a steady solution of the system (1) -(3) at 5 = 0. Assume also that a t R = R, the solution is unstable with respect to the disturbances of the frequency w,, and a t R > R, there is a soft nonlinear development of instability which relax t o a secondary autovibrational regime.…”