trinidefender wrote:I agree. Now let's relate this an F1 wing. Formula 1 has the unique situation where the low pressure side on rear wing wing is a closed loop. It is most similar to a closed loop wing. I'll find an article that I am currently working through on non-planar wing systems. The high pressure side has some restriction to span wise flow in the form of the endplates, endplate slots and on some teams wings, wing fences.
The wing is not considered infinite wingspan, just the formulas have to be changed slightly to encompass the fact that the low pressure side of the wing is a closed loop.
Correct, the presence of the endplates does significantly restrict this high pressure to low pressure flow migration, but it does not completely restrict it. In addition, with the presence of the DRS activation structure, there is a decent amount of spanwise flow, even for a low AR wing.
There are very defined experimentally found equations for the addition of endplates to performance of finite AR wings. These are typically for generic shapes, depending on who studied them.
It ranges from rectangular to elliptical endplates of differing AR. And yes, there are e values for closed wings (don't have my class notes on me, but i think it's something to do with Prandtl's wing box).
Unfortunately for F1, regulations prevent the endplate from rising much higher than the trailing edge of the last element.
McBeath has shown that that regulation loses some performance.
For some of the more complicated endplates of F1, I don't believe a singular equation can define the performance of the wing. These have heavy scalloping, and aren't constant geometry all the way down.
IMO, you need CFD/testing to evaluate a design on a case by case basis.
Remember, these wings are not fully closed in the sense of a wing box. Whatever is on the bottom of these wings varies depending on each teams suspension/diffuser/gearbox layout
There's a tradeoff here of reducing induced drag and increasing skin friction drag.