Quote:
Originally Posted by Brian Carlton
You're referring to the loss created by the frictional losses in the tires. ".
|
No, not the frictional losses, if I understand you correctly. I'm obviously having difficulty in being clear, which is my fault. Imagine that one has a steel wheel which has a flat spot similar to the radial where wheel meets flat road, level grade. But, the steel wheels geometry doesn't change from flat surface to circle instantaneously. So, we begin to roll this steel wheel forward. We first have some difficulty (power = X), then as we hit pure circle geometry we only have the rolling resistance, with all the variables that contribute to that rolling resistance (here Power to roll the wheel = X-a, where "a" is some constant). In the rubber radial, I think, we have the same basic phenomenon going. Though, with the caveat that the first non-flat spot is also circular (for some small distance) but that arc belongs to a circle of much greater diameter than our 20" diameter (for example) wheel. That arc always just ahead of the flat spot belonging to a circle diameter of >20", which in a continuous fashion moves towards the arc belonging to the 20" diameter circle uses some of the power put to the wheel by the axel. This is the basis by my saying the tire of relatively non-rigid geometry is essentially always going "uphill" in the same manner as if the relatively rigid steel wheel "experiences" going uphill, though the radial does it all of the time and the steel wheel only goe's uphill when the road grade is uphill. I do understand that even in my analogy that the flexing rubber has it's own intrinsic frictional loss as it rolls. apologize for moving towards a point, correct or not, that moves perhaps too far away from Post #1. I agree, Duke has provided us with the mathematical versus the intuitive physics, which is invaluable.