POSTER

In the process, we found out that the upper branch displays the features of turbulent large-scale coherent motions and can be continued into a coherent solution to filtered

Studying the spanwise velocity at the channel centerline, Henningson and Kim 18 observed that there is a mean motion out from the spot toward the wing tips and that this outward

We have formulated a nonlinear variational framework in order to identify control strategies (in terms of initial perturbations or boundary conditions) optimising either

The fact that for all the three types of response, the maximum energy amplification is obtained by streamwise uniform structures (α = 0) is in accordance with the sim- ilar analyses

- The Poiseuille cell was formed by two parallel lucite plates polished to provide the molecular alignment (Fig. Parallel metallic wires of uniform diameter d = 200

fixed δ ∗ ) while the latter describes a temporal boundary layer flow (i.e.. These equations are associated with homogeneous boundary conditions at the wall and at the upper

However, since we are interested in the simultaneous minimization of two quantities, that is the drag and kinetic energy density of the flow, we propose to design a control law based

The present LES results are compared to the velocity measurements of Nouri and Whitelaw [5] and to the LES of Chung and Sung [2] for three values of the rotation parameters N =