I guess what I was really trying to say here was that according to friction
circle theory (from what I thought I got out of it, anyway), if the tire's
maximum force is being applied along the tire's longitudinal axis, there is
none left for lateral force. Matt indicated that he liked to include some
lateral force anyway, because otherwise there can be very strong yawing
tendencies. With 0 lateral force at the rears, you can spin around rather
quickly. For instance, if the tire's spinning wildly, at 100 slip ratio, all
the available force should be applied along the longitudinal axis according to
what little I've read on friction circle use. I agreed with his approach,
saying it would probably be best for me to go ahead and allow a small amount of
lateral force anyway.
That's already included in my model when calculating the instantaneous
direction of each tire, before finding the tire heading, and before subtracting
the two to find the slip angle.
By "a component", you mean the lateral component. I think I see what you're
doing. You're letting the velocity vector define the total available force
(and possibly limiting it if it gets too big), then braking it into lateral and
longitudinal components if you want to analyze those seperately. This way,
even a wildly spinning tire that has some slip angle/lateral movement will
produce a lateral force. That's interesting. Different from what I'm doing.
I'll ponder that awhile :0)
Todd Wasson
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