Continuing from above, the grey bands represent the interface between the turbulent region denoted by the black vortex and the inflow. What goes on in that interface, and how broad it would be, would depend on the inflow conditions.vonk wrote: I think there’s general agreement that the air entering the diffuser will do so at speeds/pressures that vary with the speed of the car. But the exit condition is always the ambient static pressure in the car’s wake.
So, regardless of the philosophy by which one arrives at the inflow conditions, the diffuser must always have a matching area ratio to avoid back flow. A fixed wall diffuser can’t do that.
The following drawings depict three expansion conditions that might be expected in a concave diffuser (if it works).
But it’s late and I’m going to bed. Good night, I’ll talk to you tomorrow.
As I mentioned before, all of this is highly conjectural on my part. To what degree is the inflow at B laminar? Will an interface actually develop, or will the inflow burst into turbulence the moment it enters the diffuser. Is “diffuser” a misnomer for this device? Since it is the equivalent of “backflow”, the turbulent region would be at ambient pressure, though.
Somebody else must have asked the same question and the found it worth a try.


vonk