On the book “Dall’aerodinamica alla potenza in Formula 1” written by Enrico Benzing, there are examples of some curves optimised for diffuser, here the equations :
A1 : y(x) = .233 x + 1.084 10^-5 x^2 + 1.261 10^-5 x^3 – 2.735 10^-9 x^4
B1 : y(x) = .14 x + 1.282 10^-3 x^2 – 1.225 10^-5 x^3 + 1.401 10^-7 x^4
C1 : y(x) = 6.642 10^-2 x + 1.734 10^-3 x^2 – 2.15 10^-5 x^3 + 1.866 10^-7 x^4
A2 : y(x) = .131 x + 1.204 10^-3 x^2 - 1.725 10^-5 x^3 + 2.711 10^-7 x^4
B2 : y(x) = 5.203 10^-2 x + 2.51 10^-3 x^2 – 4.953 10^-5 x^3 + 4.725 10^-7 x^4
C2 : y(x) = 1.514 10^-2 x + 1.294 10^-3 x^2 – 2.544 10^-5 x^3 + 3.149 10^-7 x^4
All have a slope in the first part of about 5-7°. Then diffusers of the group 1 are more linear while group 2 have a more evident curvature. The letter identifies the height at the trailing edge in % of diffuser length, about 35% (A), 26-27% (B) and 20% (C).
Obviously for the inlet section you can be way more “brutal”, flow is accelerating there, no risk of separation.
Hope this helps as starting point.
Mikey_s wrote:
From your picture you have a venturi at the front of the car and then the opposite shaped venturi as the diffuser. Without running CFD on the model I can imagine that you are going to get a high pressure area at the narrowest point of the "inlet" venturi which will work against you at the front end of the car. In a typical F1 vehicle the air is intriduced under the car by a splitter, a "sharp", straight line whch separates the flow in a nice clean fashion. Therafter the undertray slopes gently upwards thereby increasing the volume under the car which leads to a gradual negative pressure gradient. When you get to the back end of the car the diffuser then increases the volume dramatically, thereby leading to a large(r) pressure drop - providing it doesn't stall.
Mikey, you have it all backwards, aerodynamics doesn’t work based on P V = n R T hence = constant for a given temp. We are not talking about a closed environment so air can’t enter or get out hence the given number of gas molecules will occupy the space so you have a variation of density (hence) pressure depending by the variation of volume.
In aerodynamics mass conservation means that the mass of fluid entering in a given duct (real as a tunnel or virtual as a streamtube) has to be equal to the mass of fluid getting out => to any section of the duct you have to apply the relationship rho * area * v = constant, where rho is the density, Area is the cross sectional area of the element and v is the speed of the airflow.
At low speed (under Mach = 0.3) the flow is incompressible meaning that density is constant so you have => Area * v = constant.
Then where velocity is high pressure is low and viceversa (in a very ideal case, when a quantity of hypothesis are valid, then you can apply the famous Bernouilli equation p + 0.5 rho v^2 = constant).
Consequently in the narrowest point at the front, since the area is lower, velocity will be higher and consequently pressure lower. In the diffuser then area is increasing so speed is decreasing hence you have a positive pressure gradient leading to the increment of pressure from the low pressure under the car to the high pressure present at the trailing edge.
Read my post in the following thread, I explained with more details the basics of how the underfloor works :
viewtopic.php?t=3277&start=15