Here the speed vs time of Massa’s first chicane braking at Monza during the qualifying lap. Black is what I obtained from this lap (
http://www.youtube.com/watch?v=VcUGC_GoVnc) and green is a 3rd order polynomial approximation I used for the calculation :
[IMG:150:128]http://img56.imageshack.us/img56/4339/s ... or6.th.jpg[/img]
And that’s consequently the acceleration vs speed :
[IMG:150:128]http://img146.imageshack.us/img146/4884 ... tq5.th.jpg[/img]
Now a few educated guesses about the parameters.
Mass 625 kg (Massa stopped on lap 19 hence at that point in qual had probably 8-9 laps of fuel, 25 kg sounds about right as fuel load)
Wheelbase 3 m.
Static weight distribution F/R 0.43/0.57
CG height 0.23 m. (that’s what I heard from a reliable source about 3 years ago)
Density = 1.15 kg/m3 (according to data I have temp was about 28-30°C and pressure 1003 mbar)
SCd = 0.8 m2
(meaning top speed 346 km/h needs about 580 hp only for aero, adding the roughly 100-120 for rolling resistance and the transmission efficiency we should be more or less in the ballpark of current F1 engine power)
Efficiency = 3
Static aero distribution F/R 0.4/0.6 (I’ll consider it constant during the braking)
Using these parameters and the velocity vs time I calculated a first order approximation of vertical load distribution on the wheels, from the moments of weight, inertial force and downforce. I didn’t consider the moment generated by aero drag because honestly I have no idea where an equivalent centre of pressure would be in term of height. Nevertheless consider that that moment goes in the opposite direction compared with the moment of inertial force so if anything it would reduce load at the front.
Here the result of vertical load percentage at the front as function of speed :
[IMG:150:128]http://img56.imageshack.us/img56/8292/s ... nc8.th.jpg[/img]
Obviously that’s a first order approximation but shouldn’t be off by much, I tried different simulations varying the parameters I’m less sure of and keeping them in reasonable range the result didn’t change by much, peak varying by 2-3% at max.
Even using “crazy” data for the parameters the result is most sensible to, as for example a very high 0.3 m for cg height and efficiency as low as 1.5 (hence half the downforce estimated in the above example) the maximum load at the front was always under 65%.
At the end an interesting thing I noticed when I went to the track the Friday of the Gp, watching GP2 cars at the first chicane it was quite usual to see the blockage of the rear wheel :
[IMG:150:128]http://img269.imageshack.us/img269/3591 ... qy2.th.jpg[/img]
(something that in F1 you hardly see since the throttle is carefully controlled to use the engine like sort of ABS for rear wheels).
In fact it’s impressive the difference in the “strategy” to attack the chicane between F1 and GP2 cars, it’s difficult to explain (particularly in English...), but GP2 included lot more sliding, it was like a smooth continuous action with the impression that the driver was about to lose it any moment, while for F1 cars it was more “stop & go” and with the rear end constantly glued to the track. The impression of “stop & go” is then enhanced by the fact that in the central part of the chicane F1 cars have tremendous traction in spite of the low speed, the car gains km/h in very few meters while GP2 cars don’t have a similarly brutal acceleration so between the right and left turn there’s no the evident change of speed and that contributes to make the whole action smoother.
gcdugas wrote:
For that matter, were it possible to place the CG below the fromt axle height, there would be weight transfer to the rear under braking. And in an ideal world if the CG is at exactly (or within a cm or so) of the front axle height, there would be no weight transfer.
Last time I checked the braking forces were applied at the tyres contact patch, hence at the ground, not at wheel axle.
This mean that what you say above is true when the reference is the ground, not the wheel axle.
There will be always weight transfer unless the cg is at ground level, and there will be weight transfer to rear only if the CG is below the ground. Both these things not really easy to achieve...
Obviously that’s the weight transfer related only to cg position and car wheelbase. Once these parameters are set that weight transfer for a given acceleration is set.
The dive/squat is another matter altogether and is conceptually similar to roll. In presence of body movement, being it roll or pitch, you have a further weight transfer.
In braking the inertial force applied to the cg will make the body rotate around a certain point that we can call “pitch centre”, the position of this point related suspension geometry. If that point is below the CG, in braking the front of the car will point down, if the “pitch centre” is above the CG in braking the nose will point up, if the pitch centre coincides with CG the car will remain flat.
Same concept applies to acceleration and same concept applies to roll.
The whole antidive/antisquat design of suspensions is related to put the pivot of the body rotation as close as possible to CG so to minimize body movement and minimize that further weight transfer that is related to body movements.
Anyway all of that has no influence on the basic weight transfer related to car’s longitudinal/lateral acceleration, that one is absolutely independent by suspension geometry and by body movement. To reduce it there are only two things you can do, reduce CG height (and there’s no “too low” for it) or increase wheelbase/wheeltrack.