Integrate distance across a velocity reversal
Use zero crossings to distinguish signed displacement from accumulated distance.
Learning outcome: Compare T=1,2,3 and 5 at tau=2. Locate the velocity zero, integrate with signs and verify distance≥|displacement| including endpoint reversal.
Starting recap
Differentiate or integrate with stated units, initial values, event boundaries and evidence limits.
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At tau=2,T=3, displacement −3 m but distance 23/3 m; the path reverses at 2 s.
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Can a small net displacement hide a much longer route?
Experiment
Compare T=1,2,3 and 5 at tau=2. Locate the velocity zero, integrate with signs and verify distance≥|displacement| including endpoint reversal.
Split an absolute-velocity integral at a reversal
Worked teaching model · synthetic values · Prescribed v(t)=k(t²−tau²) with k=1 m/s³, x(0)=0. Distance is integral |v|; displacement is integral v. Only nonnegative times considered; endpoint and no-reversal intervals included.
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Signed velocity
Axes rescale independently. Curves join sampled coordinates; a joining segment is not additional measured evidence. Read physical units rather than screen angles or apparent slopes.
Signed velocity: numerical coordinates
| time (s) | velocity (m/s) |
|---|---|
| 0 | -4 |
| 0.1 | -3.99 |
| 0.2 | -3.96 |
| 0.3 | -3.91 |
| 0.4 | -3.84 |
| 0.5 | -3.75 |
| 0.6 | -3.64 |
| 0.7 | -3.51 |
| 0.8 | -3.36 |
| 0.9 | -3.19 |
| 1 | -3 |
| 1.1 | -2.79 |
| 1.2 | -2.56 |
| 1.3 | -2.31 |
| 1.4 | -2.04 |
| 1.5 | -1.75 |
| 1.6 | -1.44 |
| 1.7 | -1.11 |
| 1.8 | -0.76 |
| 1.9 | -0.39 |
| 2 | 0 |
| 2.1 | 0.41 |
| 2.2 | 0.84 |
| 2.3 | 1.29 |
| 2.4 | 1.76 |
| 2.5 | 2.25 |
| 2.6 | 2.76 |
| 2.7 | 3.29 |
| 2.8 | 3.84 |
| 2.9 | 4.41 |
| 3 | 5 |
| Quantity | Value | Unit |
|---|---|---|
| Signed displacement | -3 | m |
| Total distance | 7.66667 | m |
| Final velocity | 5 | m/s |
| Final acceleration | 6 | m/s² |
| Interior reversal occurs | 1 | flag |
| Reversal time | 2 | s |
Integrating velocity permits cancellation; integrating speed requires a sign-aware partition.
For T≤tau all velocity is nonpositive and distance = −displacement. For T>tau split at tau: distance = −F(tau)+F(T)−F(tau). A zero instantaneous velocity does not imply zero acceleration or zero distance traveled.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
Integrating velocity permits cancellation; integrating speed requires a sign-aware partition.
For T≤tau all velocity is nonpositive and distance = −displacement. For T>tau split at tau: distance = −F(tau)+F(T)−F(tau). A zero instantaneous velocity does not imply zero acceleration or zero distance traveled.
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Why does setting final velocity to zero not establish zero acceleration or zero journey length?
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