Abstract
A new method, enabling the computation of steady solutions of the Navier–Stokes equations in globally unstable configurations, is presented. We show that it is possible to reach a steady state by damping the unstabletemporalfrequencies. This is achieved by adding a dissipative relaxation term proportional to the high-frequency content of the velocity fluctuations. Results are presented for cavity-driven boundary-layer separation and a separation bubble induced by an external pressure gradient.
Users
Please
log in to take part in the discussion (add own reviews or comments).