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SCIENCE · INVESTIGATE AND EXPLAIN

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.

All lessons are open directly. Your saved experiments remain when you leave and return.

Try

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 experiment

Predict

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.

Reset keeps your prediction, captures and practice history.

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.

stationary floorcenter translation rightrim relative to center: leftcontact sum: -1 m/s (right positive)

Arrows are schematic component directions, not scaled magnitudes. Zero components are omitted. Friction follows the contact sum, not whichever drawn arrow looks longer.

Calculated evidence ledger — synthetic teaching model
QuantityValueUnit
Bottom contact velocity relative to floor-1m/s
Translational kinetic energy1J
Rotational kinetic energy2J
Total kinetic energy3J
Kinetic friction direction1−1 left,0 no slip diagnosed,+1 right
Accessible plot coordinates
Primary plotted points
coordinatevalue

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.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

1. Frame the question

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.

2. Build the mechanism

For a disk moving right and spinning clockwise, the bottom point’s rotational motion relative to the center is leftward. If the center moves faster than this opposing rim motion, the contact slides right and kinetic friction acts left. That friction reduces rightward translation and produces a clockwise torque, increasing clockwise spin. If the disk is overspinning so the bottom slides left, friction acts right: translation speeds up while clockwise spin slows.

The numerical snapshot optionally displays the simple velocity difference vcontact=vCM−Rω to make the qualitative diagnosis explicit. AP Physics 1 requires the qualitative changes, not a quantitative time evolution or transition-time calculation for slipping. The tool deliberately does not integrate frictional motion or model rolling resistance.

Kinetic friction opposes relative contact motion and dissipates mechanical energy even when it increases the translational kinetic-energy part. In the overspinning case, a larger rotational-energy decrease can accompany a smaller translational-energy increase. At an instant with no slip, do not assign a kinetic-friction direction; static friction, if any, depends on other forces and constraints.

3. Work an example

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.

4. Predict and investigate

Predict first: Can friction increase a body’s center-of-mass speed while total mechanical energy decreases?

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. Retain settings and raw evidence in the lesson notebook.

5. Transfer and explain

Try a new practice case

As a diagnostic only, a disk has R=0.2 m, center speed 3 m/s right and clockwise spin 10 rad/s. Find signed contact speed, right positive.

This extra practice is not saved and does not award mastery. Record your first answer, explanation and whether you revealed help in the lesson notebook. Use the lesson’s saved question separately.

6. Reflect and retain evidence

Why is “friction always opposes the center’s velocity” an unreliable rule for a spinning body?

Retain your first response, system and axis choices, separate scalar energy and signed angular-momentum ledgers, assumptions and a changed-case prediction. Public worked checks are practice, not independent mastery evidence. Synthetic captures are not a performed physical experiment.

Framework and source notes

Original teaching prose and numerical cases. College Board AP Physics 1 CED, Unit 6 topic mapping: 6.5. Checked 30 October 2026. Planar signed analysis without required three-dimensional angular-momentum direction. Slipping evolution is qualitative, in accordance with the framework boundary; no rolling-resistance model. Framework cross-reference, not AP authorization.

Apply

A right-moving disk is overspinning so its bottom contact slides left relative to the floor. Kinetic friction on the disk points:

Public practice checks a specific claim. It does not establish independent mastery.

Why is “friction always opposes the center’s velocity” an unreliable rule for a spinning body?

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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