Identify the direction of friction from contact motion
A rotating body can slide at its contact while its center moves forward. The no-slip relation vCM=Rω is a constraint to test, not a universal identity. To reason about friction, compare the instantaneous contact motion relative to the surface, not just the direction of the center’s motion.
Learning outcome: Hold clockwise spin at 10 rad/s and compare center speeds 1, 2 and 3 m/s. Draw the center and rim contributions at contact, identify overspin/no-slip/underspin and predict the qualitative changes to translation and spin. Do not infer a transition time from this instantaneous snapshot.
Starting recap
Review axis-specific inertia, force application locations, torque-angle versus torque-time area, energy conservation and system boundaries.
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For radius 0.2 m, center speed 1 m/s and clockwise spin 10 rad/s, the bottom rotational speed relative to the center is 2 m/s left. Contact therefore slips left at 1 m/s and friction acts right. With m=2 kg and I=0.04 kg m², the instantaneous energies are 1 J translation and 2 J rotation, but those two totals do not by themselves specify a later state.
Open the experimentPredict
Can friction increase a body’s center-of-mass speed while total mechanical energy decreases?
Experiment
Hold clockwise spin at 10 rad/s and compare center speeds 1, 2 and 3 m/s. Draw the center and rim contributions at contact, identify overspin/no-slip/underspin and predict the qualitative changes to translation and spin. Do not infer a transition time from this instantaneous snapshot.
Diagnose contact slip without imposing a rolling constraint
Worked teaching model · synthetic values · Instantaneous rigid disk of mass2 kg,radius0.2 m and supplied I=.04 kg m² on a stationary horizontal surface. If contact slips, kinetic friction opposes contact motion. Only the instantaneous velocity diagnostic and energy subtotal are computed; no quantitative slipping evolution or rolling-resistance model.
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Contact velocity: add translation and local rim motion
Center translation is 1 m/s right. The bottom rim moves 2 m/s left relative to the center. Their sum at contact is -1 m/s, right positive. Kinetic friction acts right.
Arrows are schematic component directions, not scaled magnitudes. Zero components are omitted. Friction follows the contact sum, not whichever drawn arrow looks longer.
| Quantity | Value | Unit |
|---|---|---|
| Bottom contact velocity relative to floor | -1 | m/s |
| Translational kinetic energy | 1 | J |
| Rotational kinetic energy | 2 | J |
| Total kinetic energy | 3 | J |
| Kinetic friction direction | 1 | −1 left,0 no slip diagnosed,+1 right |
Accessible plot coordinates
| coordinate | value |
|---|
Contact slips left: friction acts right, increasing rightward translation and reducing clockwise spin.
vCM=Rω is a no-slip constraint, not an identity valid for every rotating body. Kinetic friction opposes relative contact motion rather than automatically opposing center-of-mass motion. During slipping it converts mechanical energy to thermal/internal energy; this model does not calculate the later transition time.
Contact slips left: friction acts right, increasing rightward translation and reducing clockwise spin.
vCM=Rω is a no-slip constraint, not an identity valid for every rotating body. Kinetic friction opposes relative contact motion rather than automatically opposing center-of-mass motion. During slipping it converts mechanical energy to thermal/internal energy; this model does not calculate the later transition time.
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Why is “friction always opposes the center’s velocity” an unreliable rule for a spinning body?
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