Split a motion interval at its actual reversal
Negative acceleration does not always mean decreasing speed. With positive initial velocity, a negative acceleration first slows the object. If the same acceleration continues after velocity reaches zero, the object moves increasingly fast in the negative direction. The model must say whether a controller stops the process at rest; this one does not.
Learning outcome: Compare v0=3,4,5 m/s at b=1, then compare b=1 and 2 at v0=3. Retain the event time, interval classification and separately calculated distance/displacement. Explain why extrapolating after 4 s requires another model claim.
Starting recap
Use SI units, signed components, algebraic ratios and graph coordinates. Identify the measurement rule and distinguish a record from an interpolated model.
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Try
At v0=4 m/s and b=1 m/s², zero velocity occurs exactly at 4 s. The object travels 8 m forward, ends at x=10 m and has no backward travel within the modeled interval.
Open the experimentPredict
Does reaching zero velocity at the final instant require adding a backward distance?
Experiment
Compare v0=3,4,5 m/s at b=1, then compare b=1 and 2 at v0=3. Retain the event time, interval classification and separately calculated distance/displacement. Explain why extrapolating after 4 s requires another model claim.
Separate distance and displacement across a reversal
Worked teaching model · synthetic values · Starts at x=2 m and v0>0, constant acceleration−b for a full4 s; no controller stops the motion at reversal. Uniform acceleration is assumed only in that declared interval. Mathematical point motion, not a stopping-distance safety rule.
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Position and exact reversal boundary
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: constant-acceleration position (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Position and exact reversal boundary
constant-acceleration position
| time (s) | position (m) |
|---|---|
| 0 | 2 |
| 0.05 | 2.1475 |
| 0.1 | 2.29 |
| 0.15 | 2.4275 |
| 0.2 | 2.56 |
| 0.25 | 2.6875 |
| 0.3 | 2.81 |
| 0.35 | 2.9275 |
| 0.4 | 3.04 |
| 0.45 | 3.1475 |
| 0.5 | 3.25 |
| 0.55 | 3.3475 |
| 0.6 | 3.44 |
| 0.65 | 3.5275 |
| 0.7 | 3.61 |
| 0.75 | 3.6875 |
| 0.8 | 3.76 |
| 0.85 | 3.8275 |
| 0.9 | 3.89 |
| 0.95 | 3.9475 |
| 1 | 4 |
| 1.05 | 4.0475 |
| 1.1 | 4.09 |
| 1.15 | 4.1275 |
| 1.2 | 4.16 |
| 1.25 | 4.1875 |
| 1.3 | 4.21 |
| 1.35 | 4.2275 |
| 1.4 | 4.24 |
| 1.45 | 4.2475 |
| 1.5 | 4.25 |
| 1.55 | 4.2475 |
| 1.6 | 4.24 |
| 1.65 | 4.2275 |
| 1.7 | 4.21 |
| 1.75 | 4.1875 |
| 1.8 | 4.16 |
| 1.85 | 4.1275 |
| 1.9 | 4.09 |
| 1.95 | 4.0475 |
| 2 | 4 |
| 2.05 | 3.9475 |
| 2.1 | 3.89 |
| 2.15 | 3.8275 |
| 2.2 | 3.76 |
| 2.25 | 3.6875 |
| 2.3 | 3.61 |
| 2.35 | 3.5275 |
| 2.4 | 3.44 |
| 2.45 | 3.3475 |
| 2.5 | 3.25 |
| 2.55 | 3.1475 |
| 2.6 | 3.04 |
| 2.65 | 2.9275 |
| 2.7 | 2.81 |
| 2.75 | 2.6875 |
| 2.8 | 2.56 |
| 2.85 | 2.4275 |
| 2.9 | 2.29 |
| 2.95 | 2.1475 |
| 3 | 2 |
| 3.05 | 1.8475 |
| 3.1 | 1.69 |
| 3.15 | 1.5275 |
| 3.2 | 1.36 |
| 3.25 | 1.1875 |
| 3.3 | 1.01 |
| 3.35 | 0.8275 |
| 3.4 | 0.64 |
| 3.45 | 0.4475 |
| 3.5 | 0.25 |
| 3.55 | 0.0475 |
| 3.6 | -0.16 |
| 3.65 | -0.3725 |
| 3.7 | -0.59 |
| 3.75 | -0.8125 |
| 3.8 | -1.04 |
| 3.85 | -1.2725 |
| 3.9 | -1.51 |
| 3.95 | -1.7525 |
| 4 | -2 |
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.
Signed velocity
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: velocity (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Signed velocity
velocity
| time (s) | velocity (m/s) |
|---|---|
| 0 | 3 |
| 4 | -5 |
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 |
|---|---|---|
| Final position | -2 | m |
| Signed displacement | -4 | m |
| Path distance | 8.5 | m |
| Final signed velocity | -5 | m/s |
| Average velocity | -1 | m/s |
| Average speed | 2.125 | m/s |
| Time of zero velocity in continued model | 1.5 | s |
| Reversal strictly inside interval | 1 | flag |
Distance requires splitting at a reversal; displacement is just the final minus initial position.
The zero-velocity event is t=v0/b. If it lies after4 s, no reversal occurs in the observed interval; if exactly at4 s, arrival is a zero-speed endpoint, not an extra backward segment. Negative acceleration can first reduce speed and later increase it in the negative direction.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Distance requires splitting at a reversal; displacement is just the final minus initial position.
The zero-velocity event is t=v0/b. If it lies after4 s, no reversal occurs in the observed interval; if exactly at4 s, arrival is a zero-speed endpoint, not an extra backward segment. Negative acceleration can first reduce speed and later increase it in the negative direction.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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How can an object have negative average velocity but positive average speed?
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