Apologies for the lack of communication recently.
Dipesh1995 wrote: ↑11 Sep 2017, 20:04
I made some minor changes to the wing around the tunnel vortex serrations and the leading two elements of the wing but none of those parts don't really influence the Y250. The vortex leaving the inboard tips is the same.
Given that the main premise of the edge vortex is to blast the front surface of the rotating tyre to try and minimize the 6 vortices being shed by it, if youre playing around with anything in that area, you may have upset the system from what you had before and its now no longer doing that.
I would also strongly recommend you ALWAYS begin your simulations from timestep zero with a full initialization, rather than continuing from current data; especially if you are changing geometry and thus your mesh!!
Dipesh1995 wrote: ↑14 Sep 2017, 17:50
Anyway, I ran the sim again but this time with the full wing with small reduction in AoA of the flap to get rid of trailing edge separation. The planform Cl value I got was -2.15 and the planform Cd I got was 0.14. The planform area of the wing is 1.214 m^2.
You mentioned planform area? In my experience, the way that Cd and Cl are used in motorsport is based on the frontal area rather than the planform area. Aviation use planform area, however, racing tends to use the same area figure (frontal usually) for both lift and drag. Also, teams often wont even use a specific frontal area due to the fact it changes with all the little tweaks that they make to the wing pitches, rake angles, etc etc... They will often just use a "standard constant" value for all calculations to keep things homogenous.
Dipesh1995 wrote: ↑16 Sep 2017, 11:38
1. Realizable K-Epsilon, as seen for wing simulations, tends to overestimate lift coefficients by roughly 9-10% and sometimes even more compared to experimental results.
I would agree with the over-estimation with regards to the standard k-eps model as it has been shown experimentally to break down when measured next to complex gemetries with strong adverse pressure gradients (i.e. wings in ground effect). The realizable k-eps model though is slightly different in that it uses a changeable variable for the C(mu) value rather than a constant. It also has a new transport equation for the dissipation rate which comes from an exact differential equation derviation; these two things means that it is substantially better at modelling complex geometries, boundary layer shear/flows, strong adverse pressure gradients, etc, than its standard version. There are obviously better turbulence models out there for this specific type of thing, but it isn't all that bad.
Dipesh1995 wrote: ↑16 Sep 2017, 11:38
Anyway, I'm now going to start to wind this down as I need to turn my attention to my FYP. Once again, I really do appreciate the help you and Vyssion have given me throughout these last couple of months.
You're welcome mate.
Always welcome back with your new questions etc!