Close a thermal ledger at the actual stopping point
A 2 kg point begins at 4 m/s on a level surface, so its kinetic energy is 16 J. A constant kinetic friction magnitude f opposes motion. For the point alone, friction work over actual forward distance d is−fd, giving K=16−fd. This equation is valid only while that forward sliding branch exists.
Learning outcome: Compare requested distances1,2,4 m at friction 6 N, then double or halve friction where controls permit. Record requested versus actual distance and show both the point-only and object-plus-surface accounts without double-counting.
Starting recap
Choose the system, interval and reference frame before using a conservation statement. Keep vector momentum, scalar energy and transferred power distinct.
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For f=8 N and requested distance 2 m, the endpoint is exactly the stop, with zero kinetic energy and 16 J thermal gain. Equality is reached; it is not an extra post-stop interval.
Open the experimentPredict
After the unforced point stops on the level surface, this model predicts:
Experiment
Compare requested distances1,2,4 m at friction 6 N, then double or halve friction where controls permit. Record requested versus actual distance and show both the point-only and object-plus-surface accounts without double-counting.
End the sliding energy ledger at the first stop
Worked teaching model · synthetic values · A 2 kg point starts rightward at 4 m/s on a level surface. Constant kinetic friction is the only horizontal force until it stops; afterward there is no drive and it remains at rest. Thermal gain belongs to the selected object-plus-surface system.
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Sliding energy before the first stop
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: accessible sliding energy (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Sliding energy before the first stop
accessible sliding energy
| traveled distance (m) | kinetic energy (J) |
|---|---|
| 0 | 16 |
| 0.0666667 | 15.6 |
| 0.133333 | 15.2 |
| 0.2 | 14.8 |
| 0.266667 | 14.4 |
| 0.333333 | 14 |
| 0.4 | 13.6 |
| 0.466667 | 13.2 |
| 0.533333 | 12.8 |
| 0.6 | 12.4 |
| 0.666667 | 12 |
| 0.733333 | 11.6 |
| 0.8 | 11.2 |
| 0.866667 | 10.8 |
| 0.933333 | 10.4 |
| 1 | 10 |
| 1.06667 | 9.6 |
| 1.13333 | 9.2 |
| 1.2 | 8.8 |
| 1.26667 | 8.4 |
| 1.33333 | 8 |
| 1.4 | 7.6 |
| 1.46667 | 7.2 |
| 1.53333 | 6.8 |
| 1.6 | 6.4 |
| 1.66667 | 6 |
| 1.73333 | 5.6 |
| 1.8 | 5.2 |
| 1.86667 | 4.8 |
| 1.93333 | 4.4 |
| 2 | 4 |
| 2.06667 | 3.6 |
| 2.13333 | 3.2 |
| 2.2 | 2.8 |
| 2.26667 | 2.4 |
| 2.33333 | 2 |
| 2.4 | 1.6 |
| 2.46667 | 1.2 |
| 2.53333 | 0.8 |
| 2.6 | 0.4 |
| 2.66667 | 0 |
At most 82 representative computed coordinates including endpoints; the plotted curve can use a finer grid. A table of a revealed generator is not independent measurement evidence.
| Quantity | Value | Unit |
|---|---|---|
| Initial kinetic energy | 16 | J |
| Stop distance | 2.66667 | m |
| Actual traveled distance | 2.66667 | m |
| Requested endpoint reached | 0 | flag |
| Friction work on point | -16 | J |
| Object-plus-surface thermal gain | 16 | J |
| Remaining kinetic energy | 0 | J |
| Endpoint speed | 0 | m/s |
Mechanical energy decreases while the larger object-plus-surface energy account remains closed.
Kinitial=16 J and friction removes f d until dstop=16/f. Beyond that event the point stays still without a drive, so there is no extra sliding or additional friction heating. Do not subtract friction work and add the same thermal gain as two separate losses in the same system account; they describe the transfer using different boundaries.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Mechanical energy decreases while the larger object-plus-surface energy account remains closed.
Kinitial=16 J and friction removes f d until dstop=16/f. Beyond that event the point stays still without a drive, so there is no extra sliding or additional friction heating. Do not subtract friction work and add the same thermal gain as two separate losses in the same system account; they describe the transfer using different boundaries.
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Which system boundary makes thermal gain an internal energy change rather than an omitted transfer?
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