Integrate acceleration twice and locate a reversal
Acceleration alone does not specify one unique trajectory.
Learning outcome: Compare an interval ending before reversal, exactly at reversal where supported, and after it. Preserve both integration constants and piecewise distance calculations.
Starting recap
Read derivatives as local rates and integrals as signed accumulation. Review power and chain rules, vector components, units and initial conditions where used.
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Try
With α=2 and T=2, v=2 m/s, x=−1/3 m and displacement−4/3 m. Reversal is sqrt2 s; distance is(8sqrt2−4)/3≈2.43790 m.
Open the experimentPredict
For α=1 from t0 to4 s, the traveled distance is:
Experiment
Compare an interval ending before reversal, exactly at reversal where supported, and after it. Preserve both integration constants and piecewise distance calculations.
Recover two initial conditions and a reversal
Worked teaching model · synthetic values · One-dimensional prescribed a(t)=αt, initial velocity−2 m/s and position1 m. No forces or drag are inferred. Distance uses the absolute velocity integral split at its nonnegative zero, not absolute displacement.
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Integrated position with both initial conditions
Unlike graph quantities rescale independently; read units and values, not screen angles. 1: x0+integral of velocity (solid). Joined curves show the supplied model, not additional observations.
Equivalent numerical coordinates for Integrated position with both initial conditions
x0+integral of velocity
| time (s) | position (m) |
|---|---|
| 0 | 1 |
| 0.05 | 0.9000208 |
| 0.1 | 0.8001667 |
| 0.15 | 0.7005625 |
| 0.2 | 0.6013333 |
| 0.25 | 0.5026042 |
| 0.3 | 0.4045 |
| 0.35 | 0.3071458 |
| 0.4 | 0.2106667 |
| 0.45 | 0.1151875 |
| 0.5 | 0.02083333 |
| 0.55 | -0.07227083 |
| 0.6 | -0.164 |
| 0.65 | -0.2542292 |
| 0.7 | -0.3428333 |
| 0.75 | -0.4296875 |
| 0.8 | -0.5146667 |
| 0.85 | -0.5976458 |
| 0.9 | -0.6785 |
| 0.95 | -0.7571042 |
| 1 | -0.8333333 |
| 1.05 | -0.9070625 |
| 1.1 | -0.9781667 |
| 1.15 | -1.046521 |
| 1.2 | -1.112 |
| 1.25 | -1.174479 |
| 1.3 | -1.233833 |
| 1.35 | -1.289938 |
| 1.4 | -1.342667 |
| 1.45 | -1.391896 |
| 1.5 | -1.4375 |
| 1.55 | -1.479354 |
| 1.6 | -1.517333 |
| 1.65 | -1.551312 |
| 1.7 | -1.581167 |
| 1.75 | -1.606771 |
| 1.8 | -1.628 |
| 1.85 | -1.644729 |
| 1.9 | -1.656833 |
| 1.95 | -1.664187 |
| 2 | -1.666667 |
| 2.05 | -1.664146 |
| 2.1 | -1.6565 |
| 2.15 | -1.643604 |
| 2.2 | -1.625333 |
| 2.25 | -1.601563 |
| 2.3 | -1.572167 |
| 2.35 | -1.537021 |
| 2.4 | -1.496 |
| 2.45 | -1.448979 |
| 2.5 | -1.395833 |
| 2.55 | -1.336438 |
| 2.6 | -1.270667 |
| 2.65 | -1.198396 |
| 2.7 | -1.1195 |
| 2.75 | -1.033854 |
| 2.8 | -0.9413333 |
| 2.85 | -0.8418125 |
| 2.9 | -0.7351667 |
| 2.95 | -0.6212708 |
| 3 | -0.5 |
| 3.05 | -0.3712292 |
| 3.1 | -0.2348333 |
| 3.15 | -0.0906875 |
| 3.2 | 0.06133333 |
| 3.25 | 0.2213542 |
| 3.3 | 0.3895 |
| 3.35 | 0.5658958 |
| 3.4 | 0.7506667 |
| 3.45 | 0.9439375 |
| 3.5 | 1.145833 |
| 3.55 | 1.356479 |
| 3.6 | 1.576 |
| 3.65 | 1.804521 |
| 3.7 | 2.042167 |
| 3.75 | 2.289063 |
| 3.8 | 2.545333 |
| 3.85 | 2.811104 |
| 3.9 | 3.0865 |
| 3.95 | 3.371646 |
| 4 | 3.666667 |
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 velocity | 6 | m/s |
| Final position | 3.666667 | m |
| Signed displacement | 2.666667 | m |
| Traveled distance | 8 | m |
| First velocity reversal time | 2 | s |
| Reversal occurs in selected interval | 1 | flag |
Integrating acceleration twice requires two independently specified initial conditions.
v=−2+αt²/2 and x=1−2t+αt³/6. Integrate absolute velocity in separate sign intervals to find distance. The positive zero sqrt(4/α) may lie beyond the selected interval; do not insert an unobserved reversal or confuse the integration constant with a force parameter.
Predict before inspecting the values. Save contrasting records with assumptions and one alternative explanation. This virtual display does not certify practical measurement technique.
Integrating acceleration twice requires two independently specified initial conditions.
v=−2+αt²/2 and x=1−2t+αt³/6. Integrate absolute velocity in separate sign intervals to find distance. The positive zero sqrt(4/α) may lie beyond the selected interval; do not insert an unobserved reversal or confuse the integration constant with a force parameter.
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What can and cannot be reconstructed if only acceleration, but no initial velocity, is supplied?
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