mattt
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Anyway, the example of one single wheel rolling on an horizontal ground is even more interesting.
I guess you are perplexed that if the wheel is rolling (without sliding) and the only exterior forces acting on the wheel are the weight, the normal force and the static friction force, how is it that the wheel end up stopping if the only force that causes a non-zero torque (wrt COM) is the static friction force and it "should" increase the angular velocity (the angular momentum vector) ? :-)
Or imagine you are pushing the center of mass of the wheel so that the center of mass is moving with uniform rectilinear motion. Again, the only force (apparently) that causes a non-zero torque (wrt COM ) is the static friction force and, again, it "should" increase the angular velocity (angular momentum vector), how is it that the angular velocity remains constant? :-)
As I said, this example is good enough to test many things about Newtonian mechanics. I'll leave it to you to think about it and later on I'll comment on this example. :-)
I guess you are perplexed that if the wheel is rolling (without sliding) and the only exterior forces acting on the wheel are the weight, the normal force and the static friction force, how is it that the wheel end up stopping if the only force that causes a non-zero torque (wrt COM) is the static friction force and it "should" increase the angular velocity (the angular momentum vector) ? :-)
Or imagine you are pushing the center of mass of the wheel so that the center of mass is moving with uniform rectilinear motion. Again, the only force (apparently) that causes a non-zero torque (wrt COM ) is the static friction force and, again, it "should" increase the angular velocity (angular momentum vector), how is it that the angular velocity remains constant? :-)
As I said, this example is good enough to test many things about Newtonian mechanics. I'll leave it to you to think about it and later on I'll comment on this example. :-)