rec.autos.simulators

GPL handling question--Physics model

Doug Millike

GPL handling question--Physics model

by Doug Millike » Wed, 24 May 2000 04:00:00


> But is it true that the friction coefficient (cf) reduces/increases with
> changing load (weight transfer). I've read that cf reaches a peak at optimum
> load and is lower at higher/lower loads. For something as dynamic as a
> vehicle; can load and slip angle be separated?

If one could test at "constant conditions", then I think there is a good
chance that the friction _coefficient_ will decrease with increase in load.
Of course, in reality, things are always changing when a tire is tested, I
leave it to your imagination to figure out some of the other variables that
change.....

Tire performance is certainly a function of all the operating variables,
including load and slip angle (and many other things too).  Easy to say,
very hard to actually measure and characterize.

Basic property of a rolling tire -- it tries to align with its direction
of travel.  The effect is nonlinear and of course it goes away at/above the
limit, when the tire print is fully sliding across the road.  Pics and
diagrams are in chapter 2 of our book<shameless plug!>.

-- Doug

                Milliken Research Associates Inc.

Kevin Gavit

GPL handling question--Physics model

by Kevin Gavit » Wed, 24 May 2000 04:00:00

And the absolute best of drivers can hold the car right on the point of not
quite losing it by sensing the the reduction in pnuematic trail.

Frequently refered to as the point where the steering "goes all funny."

Now if only the FF in GPL would realisticly model this.....

Kevin Gavit

GPL handling question--Physics model

by Kevin Gavit » Wed, 24 May 2000 04:00:00


Oops, I've been infected by JTW's wrong posting virus.

This was, of course, intended to go to Tony Lake's thread.

Kevin Gavit

GPL handling question--Physics model

by Kevin Gavit » Wed, 24 May 2000 04:00:00


Ah! No, no. I believe that if you could find your copy of How to Make Your
Car Handle you would find that it would say that if you add longitudinal
load it will reduce the force AVAILABLE to generate lateral load.

Therefore, again, if we are well below the limit mild braking or
acceleration won't have any effect on the arc taken by the car.

I still get the feeling, and perhaps I'm wrong, that you've got some fuzzy
ideas about slip angle and forces generated. Slip angle is part of the
mechanical means by which a tire can generate a force. This isn't at all the
same thing as saying that a particular slip angle generates a particular
force. Since the cf is dependant on slip angle, slip angle imposes a MAXIMUM
force that the tire can generate. It can split up that force in any
combination of vectors it "likes," but as long as the tire stays within the
confines of its limit it will basically keep on doing whatever it was doing.

Again, this is very simplified but well within the parameters of our
discussion.

If you are modeling a car in a turn it's very important to remember that
what you are dealing with here is a problem in ballistics. The car is a
freely moving body moving along an arc in a plane. At any given arc and
speed the loads are given. Period.

So, we have two drivers going around a skidpad at the limit. One is Gilles
Villineuve, all crossed up, the other is Alain Prost tracking like he's on
rails. Very different slip angles on these two cars, but they're both
following the same arc and the cars both experience the same load, slip
angles be damned.

Slip angles are engineer and driver adjustable.

Now, if they both track around this circle at .2 g the tires have unused
capacity, regardless of the slip angles. This unused capacity can be used to
accelerate or brake. The tire generates ADDITIONAL forces, up to the limit,
to deal with the added loads.

I know I'm repeating myself ad naseum, but I don't know which idea or
combination of ideas is going to "click" for you, so I'm just throwing all
the speghetti against the wall here.

JTW620

GPL handling question--Physics model

by JTW620 » Thu, 25 May 2000 04:00:00

Subj:   Re: Missing r.a.s. post
Date:   5/24/00 8:14:46 AM US Mountain Standard Time
From:   JTW62074
To:     kevin...@gateway.net

        Kevin,
    I apologize for over reacting to your initial response to my post.  I do
appreciate your input.  So you understand where I'm at, here's how my model
basically works at this point:
----
   * The car is one solid mass, completely unsprung.  

        1.  The slip angles (all four tires are done seperately) are calculated based
on the positions of the wheels in relation to the center of gravity, the
vehicle's x and y velocity, rotational velocity, and steering angles.  

        2.   When these slip angles are found, the cf is computed from a simple
equation as an approximation.  The equation gives a peak cf of 1.2 in the 5-9
degree slip angle area, similar to what a Nascar tire test showed.  I realize
that the cf changes with vertical load, camber, tire pressure, temperature,
etc., at all of these slip angles, but I was keeping it simple to get the
basics down and see if my approach would work as anticipated.  Either way, this
variable is the only part of the model that needs to be updated to allow these
other factors to be taken into account.

      3.   There is no suspension model yet, so the static weight on each tire,
plus any fore/aft weight transfer and front/rear wing downforce respectively,
is multiplied by this cf to get the lateral force.  Lateral weight transfer is
not included, as there is no cf variance with vertical load in this model yet.
Since the weight transfer happens almost instantly in this model, it drives
like a car with the chassis bolted directly to the wheels and with super hard
tires (wheel rate is infinite here).

        4.    These lateral forces are then broken into x/y and rotational components
and added to wind resistance to change the x/y and rotational velocities and
postions of the car.

        5.   Loop back to 1, calculate again for the next .005 second or whatever
----
        That's basically it.  As you may see here, slip angles are determined by the
model from the motion of the car, rather than the other way around (your
explanation of the arcs a vehicle will follow is the kind of info I needed BTW,
thank you, Kevin).  In step 2, throttle and brakes are used to produce a
longitudinal force for each tire seperately.  Your approach was one of two I
had tested and it works perfectly, as far as I can tell.  It follows the paths
you described when changing longitudinal forces, and all other things happen as
you and Doug Milliken have described so far.

        Step 2 also had to limit the lateral force produced by each tire.  My "tire
model problem" was in how to do this correctly.  I thought of two methods,
yours was one of them.    

        **Method 1-Your way**-  Using your method, the total available force (in any
direction) at each tire is calculated, based on their maximum cf and total
vertical force on each tire.  Then, based on step 2 above, the lateral force at
the tire is calculated (slip angle's cf times vertical force).  The lateral and
longitudinal forces are run through the Pythagorean Theorem to limit the
lateral force if necessary, so the vector sum of the two forces will not exceed
the total traction force available (as you also described).

         So, in essence, with this lateral force limiting method, a very small slip
angle of 2 degrees producing 200 lbs of lateral force will keep producing 200
lbs of lateral force after the longitudinal force changes (unless it's enough
to exceed the total traction available at that instant, in which case the
lateral force gets limited, and the fun power slides begin).  As you said, the
car continues to follow the same arc when the longitudinal force is increased
(as long as we stay inside the total traction available).  Slip angle and
everything else will change along with it as the vehicle's speed, weight
transfer, etc., changes.  This happens automatically through the other steps
and is why I wanted to isolate the basic tire behavior from these factors to
see if the approach was basically correct.

        The method just described produces the results you spoke of.  There are no
problems with the car refusing to straighten out with throttle or brakes on,
regardless of whether the self-aligning torque model is implemented or not.  

        **Method 2**- The other lateral force limiting method, the one that would not
let the car straighten out with the throttle or brakes on even the minutest
amount, was similar.  Slip angle of a tire was calculated the same way, the cf
was calculated, and the initial lateral force was calculated for the tire the
same way.  

        Now, I read that hitting the gas in some cars while cornering causes the car
to yaw a bit more quickly (of course, my '79 Firebird didn't do this, come to
think of it), and couldn't recall from How to Make Your Car Handle exactly
whether or not this happened when the tires were nowhere near their traction
limit.  

        You pointed out that *** "...if you could find your copy of How to Make Your
Car Handle you would find that it would say that if you add longitudinal load
it will reduce the force AVAILABLE to generate lateral load." ***  
        Then the effects on yaw rate due to throttle changes (getting on the gas to
get the back end out a little more) are due to exceeding the AVAILABLE
traction, and Method 2 is incorrect.

        I thought I had read in this book that the rear slip angles changed whenever
the rear wheels were fed more torque (i.e., the lateral force was reduced by
ANY amount of longitudinal force, even though the tire wasn't near the traction
limit, therefore, the car yaws slightly more quickly for a moment, the slip
angle increases until the old lateral force returns, it stabalizes at this new
slip angle, the yaw rate slows back down a little, but the car is now following
a different arc after a brief wobble.)  As you described, this is against the
very definition of traction limit force and must be incorrect.  This also made
it impossible to straighten out the car if any throttle or brakes were applied
to the rear wheels.  

        I too, thought that using self-aligning torques would solve the problem, but
it did not.  When all the tires produced a counter-clockwise torque in a right
hand corner, the forces they produced on the center of gravity of the car more
or less cancelled each other out (depending on the geometric details of the
chassis and cg location).

        The left front tire pushed the cg forward and to the right, the front right
tire pushed the cg backwards and to the right, the rear right pushed it
backwards and to the left, and the rear left pushed it forwards and to the
left.  It does change the handling of the car slightly (not enough for me to
tell from the in-car view), but had roughly zero effect on straightening the
vehicle, even with nearly zero grip tires on the front end, so this wasn't the
problem.

        So I asked the initial GPL question, "What happens in the first instant when
you hit the gas in GPL when using the softest suspension settings?"  

        By using the softest suspension settings, the weight transfer would have very
little effect in the first couple of instants, as the springs would need to
compress and/or the dampers would need to rise in velocity in order to plant
more force on the tires (how the sprung weight's weight transfer really
happens, right?).  Of course, the unsprung weight would transfer more quickly,
but believe I could still get an idea which lateral force limiting method GPL
was using, if either, from someone's answer.  

        If someone said the car "kind of yawed in a little, wobbled, then moved
outside the turn more",  or "it turned in a little tighter at first, so I had
to back off the wheel for a split second until it set into the turn, then give
it more steering than before to keep my line", I would suspect GPL was using
something like the second method (the one that didn't let my car straighten
out).  If they said the car immediately started pushing towards the outside of
the corner, I would suspect that weight transfer caused this, and since there
was no sudden increase in yaw rate, the first method (your method) was more
correct.  

        I received one email that said  " ....[In GPL] it seems that adding gas before
nearing the traction limit simply pushes the car away from the corner without
changing it's attitude. Letting off on the gas, however, turns it in a little.
Of  course, things change when you hit the traction limit."

        This, in combination with my assumption that GPL cars can drive straight ahead
with some throttle or braking applied, unlike my model when using method 2,
tells me that your method (method 1), is more correct, just from reading this
description of GPL handling.  What this email indicates to me is that weight
transfer off the front tires and onto the rear caused it to push away from the
corner.  The attitude didn't change, so the rear slip angles probably didn't
get a sudden boost when a small amount of throttle was applied.  If the emailer
had indicated a sudden wobble and subsequent push, I'd have second thoughts.

        This answers my question, and method 1 (that follows yours and Doug Milliken's
descriptions of vehicle behavior) is now being used.  

        Cheers,
        J. Todd Wasson
http://PerformanceSimulations.Com

JTW620

GPL handling question--Physics model

by JTW620 » Thu, 25 May 2000 04:00:00

lol  My wrong posting virus is contagious!

Todd Wasson

JTW620

GPL handling question--Physics model

by JTW620 » Thu, 25 May 2000 04:00:00

>Subject: Re: GPL handling question--Physics model

>Date: 5/22/00 7:17 AM US Mountain Standard Time

>Ok, I'm sorry if I've underestimated your physics knowledge. I've only your
>questions here to go on, and I guess I'm not understanding you properly. I'm
>afraid I still don't get the feeling from your questions what you're driving
>at.

>Let's take a super simplified lab example. A large block of *** sitting
>on the concrete lab floor. Let's say it will take 200 lbs. of force to
>overcome it's cf and start it sliding across the floor.

>What happens when you push it with 50 lbs. of force?
>( I'm using 50 lbs. because it is .25 of  200, and the .2 g you use as an
>example is .25 of the cornering force a decent road car can generate.)

>Well, it pushes back with 50 lbs. of force and other than that just sits
>there.
>Push it with 100 lbs. of force and it pushes back with 100 lbs. of force and
>continues to just sit there.

>Push it with 201 lbs. of force and it will accelerate under 1 lb. of force
>by sliding across the lab floor.

>A simplfied tire does the same thing. If you only load it to .25 of it's
>force generating capacity it has a reserve capacity. Load it to .2 g at a
>real force of 200 lbs. and it is still capable of generating 600 lbs.
>additional force. Accelerate the car to .4 g and the tire responds by simply
>generating the additional force neccessary to balance the load and the car
>remains on the same arc. You can continue this right up to the limit, which
>is *defined* as the point where the arc of the car must widen to balance the
>force in accordance with the rules of circular motion. By definition if you
>are below the limit the car will follow the same arc whether you increase or
>decrease speed as long as the car stays below the limit. This is essentially
>the same way banked turns work, and why at a particular speed a car can hold
>it's wheels straight and follow a curved path with 0 side loading, using
>gravity to supply a centripital force rather than the tires. Correct? What
>about this don't you understand?

>You can go out test this on your own street car, can't you? .2 g is well
>below a speed likely to gain the interest of the authorities on turns you
>can find around any  city.

>You understand all this? So perhaps you can see my quandry at your question.
>I'm using a very simplified model here that dosn't take the fact that the
>capacity of a tire to generate force is variable with the slip angle. At .2
>g this is irrelevant to the driver because of the huge reserve capacity of
>the tire. It's only the small window around the limit that things get
>interesting, where the reserve capacity of the tire is small and may
>actually disappear. Are you being confused about the idea of slip angle and
>what it does and what it is? Am I being confused about what you are and are
>not confused about?

>The next issue  is your specific question about the reaction of GPL.

>GPL does not use a simple single tire in the lab model. It uses a model of 4
>tires attached to a semi-rigid body. It resolves the vector sum of those
>forces. How can the behaviour of such a model be used to deduce a
>hypothetical simplified single tire model? Isn't that rather like trying to
>deduce an Elephant's DNA sequence by looking at the elephant, rather than
>the other way around? I can set up a GPL car to exhibit just about any
>behaviour you want. The static loadings are user variable. Roll resistence
>is user variable. Tire pressures are user variable. Damping rates are user
>variable. All on each corner of the car seperately. Different chassis have
>different inate properties such as roll center, weight bias, suspension
>geometry, etc. Even aerodynamic properties are taken into account.

>And the arc taken by a car with 4 tires attached to it will be the vector
>sum of the forces on all four tires right? Each with a different load and
>perhaps even a different cf. Slip angle may even be different on all four
>tires depending on suspension geometry. The degree to which the arc changes
>will be the dependant on the ratio of the total slip angles of the front
>tires to the total slip angles on the rear, right? A car with larger slip
>angles at the rear will oversteer and one with larger slip angles at the
>front will understeer, correct? And the slip angles are user settable to a
>large degree, yes?

>I fail to see what you are attempting to deduce from the behaviour of GPL,
>or how you feel you can deduce anything at all by it.

>I can leave you with the same answer I gave before. In GPL if you are
>cornering at .2 g and increase your speed to .4 g the arc will change by not
>changing at all, which is exactly what it should do, and exactly what your
>street car will do.

>Can you pick up a copy of Skip Barber's Going Faster? It's available off the
>shelf at at any Borders or Barnes and Nobles, as is Van Valkenburgh's Race
>Car Engineering and Mechanics. I highly reccomend you suppliment the
>Milliken's work with these to give you a drivers perspective on the hard
>science.

>As for the car in your model not wanting to return to a straight line, have
>you modeled all the self-centering torques? A tire is a spring. When it
>moves at a slip angle it loads in torsion, and thus generates an equal and
>opposite torque. Caster and camber also need to be modeled correctly for
>their self-centering torques.

>I really have no idea whether I'm being helpful here, or just condescending.
>I MEAN to be helpful. Honest.

>Yours,

>                Kevin F. Gavitt

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Todd Wasson


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