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I’m beginning to accept that there will be an interdependence of one factor over another.There are a lot of “Dusty” corners in my knowlege that remind me how old I’m becoming. I just perceived that the stock statement of nimbleness and flickability being a function of low C of G and 3/5th’s of 5/8th’s of SFA else....Needed some examination. I like Tusayan’s approach to this stuff, he’s ahead of me but I like his approach to working man’s Physics discussions.I don’t exactly know what a curmudgeon is, but I think I’m becoming one, because I bristle a bit, when I hear illadvised or inaccurate statements trotted out blithely, accompanied by the sage nodding of heads.I’ve been pulled up here on that very issue by blokes of deeper knowlege occasionally and am the better for it.
Oh, and response #16.Duty has done a nice job, but I prefer Dusty’s take on things, although I’ll admit he does have a devotion to Duty...Also, how does one manage to get the C of G below street level ?
You and others don't need to stop asking questions, and not every answer is going to be correct.But it makes us all stop and think. And that's always a good thing.
Hell , even the *experts* have a hard time coming to a consensus on this . The fact is , what works is what works , bending the math to suit comes later . Dusty
Peter , there is a young man in the physics dept at a large state U who worked for me in college , we run these motorbike experiments every so often, he lays all of the math out , then we discuss the real world effects , then we normally laugh about all of it . Carpenter math only gets me so far The concept of raising the forks to decrease rake angle comes up once a year or so , another misunderstood concept , because when you run the math , raising the fork 26 MM reduces rake by like .2 degrees using 28 degrees as a baseline . What most riders are feeling is increased weight on the front tire from tilting the chassis , and the increased feeling of control from having their body tilted forward . Once again , motorbike physics are fun , aren't they ? Dusty
Ha ha. I corrected my typo-apologizes to DUSTY!As for GOG below street level-it was a simple graph that illustrated an intersection of various factors that determine where COG is. That intersection can be below the bike to the extent that the lines intersect below grade. It's not that hard a concept. Something tells me I saw it in Camaron's book.I'll have to dig it out and check. Nonetheless, if you understand that moment of inertia, COG, center of mass, and others are determined by vectors (I think that's it IIRC) than the concept of one or more of those measures being located above or below is not unreasonable.The entire subject sounds like a perfect topic for "Ask Kevin" at CycleWorld.
As for GOG below street level-it was a simple graph that illustrated an intersection of various factors that determine where COG is. That intersection can be below the bike to the extent that the lines intersect below grade. It's not that hard a concept. Something tells me I saw it in Camaron's book.
More likely the point below pavement was the center of rotation when the bike rocks forward and aft with braking and acceleration. Confusion may arise from the fact that a body in flight may rotate around the CoM (or CoG) (aerodynamics permitting) but a machine on the ground certainly will not.
But if you consider a bike coming head on that initiates a turn.Let us say the bike turns to (our) right, or a left hander for the rider.The wheels will be displaced to (our) left and the rider’s head will be displaced to (our) right. Somewhere in between these two points is a spot where the lateral displacement vector is zero, and that is the C of M of the system.In the case of a 130 kg rider on a 10 kg pushbike, the lateral displacement of the wheels will be considerably more than that of the rider’s head, this is because the C of M is quite high.The same rider on a wide glide with a lightweight flag above his bike to represent the same height as example #1, will exhibit a relatively small lateral movement of the wheels versus the top of the flag.This is because the C of M is very low.Guess which one is more umm.... “flickable”.
Can't agree with this. The tires are prevented from moving significantly outward from the arc by engagement with the pavement, and in fact the banking rotation has to be centered on the contact patches of the tires. Any outward movement of the front wheel -- maybe an inch or two -- is induced by the steering geometry and is what in turn induces lean angle when countersteering. I suspect the rear wheel actually tracks INSIDE the arc of the turn unless throttle-induced wheelspin breaks the traction for a power slide. Comparing steering quickness or flickability with a bicycle or push bike is unrealistic not only because of the weight differences but also because bicycles typically have a 17 degree rake and trail is at the low end of what would be acceptable with a motorcycle -- just a bit more than 2 inches.
I think some of that is a bit sketchy, but I don’t have enough raw understanding to be able to engage.The only thing I’d add, is that the engagement with the pavement is not “preventing” the tracking outside the arc, because the wider arc is initiated by the first countersteer input and that is only possible “because” of that engagement.Imagine if you were on ice and there was no engagement, the first input on the ‘bar would result if an immediate crash.The tyres are describing a larger radius than the rider’s head, gravity (downwards) is preventing the rider being thrown outwards (as if in a car), and centrifugal force (sic), is preventing the rider falling inwards due to lean, both are in equal measure.The reason I introduced the heavy rider on the light bike, was to give an example of high C of G.
Geez Peter , I explained it as simply as possible , what do you want ? Dusty
Can't agree with this. The tires are prevented from moving significantly outward from the arc by engagement with the pavement, and in fact the banking rotation has to be centered on the contact patches of the tires.
Hard countersteering can steer the tires outward from under the CG. The effect of that model is that the bike rotates around the CG, which simultaneously translates downward. The suspension extends a little until the bike settles. In actuality the bike rotates in a more complex way, somewhere between rotation around the tire patch and the CG... but I think that the harder the countersteering the closer the bike comes to rotating around the CG.