Integrate power without confusing one interaction with net work
Compare an instantaneous dot product, interval-average power and cumulative work.
Learning outcome: Compare a=1 and−1 at T=2. Derive each power curve, find any sign change and integrate signed areas. Explain what extra evidence would be needed to infer net kinetic-energy change.
Starting recap
Derive the integral or derivative, preserve the system boundary, and reject physically inaccessible continuations.
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a=1,T=2 gives W=28/3 J, average 14/3 W, endpoint 10 W. With a=−1, power crosses zero at t=1 and becomes negative afterward, while prior transferred work remains part of the interval integral.
Open the experimentPredict
Does endpoint instantaneous power generally equal interval-average power?
Experiment
Compare a=1 and−1 at T=2. Derive each power curve, find any sign change and integrate signed areas. Explain what extra evidence would be needed to infer net kinetic-energy change.
Integrate selected-interaction power over time
Worked teaching model · synthetic values · Prescribed x=t²,y=t in SI units and selected force (at,2) N. Power may change sign. Other interactions enforce the trajectory, so selected-force work is not automatically total kinetic-energy change.
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Selected instantaneous power
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.
Selected instantaneous power: numerical coordinates
| time (s) | power (W) |
|---|---|
| 0 | 2 |
| 0.05 | 2.005 |
| 0.1 | 2.02 |
| 0.15 | 2.045 |
| 0.2 | 2.08 |
| 0.25 | 2.125 |
| 0.3 | 2.18 |
| 0.35 | 2.245 |
| 0.4 | 2.32 |
| 0.45 | 2.405 |
| 0.5 | 2.5 |
| 0.55 | 2.605 |
| 0.6 | 2.72 |
| 0.65 | 2.845 |
| 0.7 | 2.98 |
| 0.75 | 3.125 |
| 0.8 | 3.28 |
| 0.85 | 3.445 |
| 0.9 | 3.62 |
| 0.95 | 3.805 |
| 1 | 4 |
| 1.05 | 4.205 |
| 1.1 | 4.42 |
| 1.15 | 4.645 |
| 1.2 | 4.88 |
| 1.25 | 5.125 |
| 1.3 | 5.38 |
| 1.35 | 5.645 |
| 1.4 | 5.92 |
| 1.45 | 6.205 |
| 1.5 | 6.5 |
| 1.55 | 6.805 |
| 1.6 | 7.12 |
| 1.65 | 7.445 |
| 1.7 | 7.78 |
| 1.75 | 8.125 |
| 1.8 | 8.48 |
| 1.85 | 8.845 |
| 1.9 | 9.22 |
| 1.95 | 9.605 |
| 2 | 10 |
| Quantity | Value | Unit |
|---|---|---|
| Selected work over interval | 9.33333 | J |
| Average selected power | 4.66667 | W |
| Instantaneous selected power at endpoint | 10 | W |
| Initial selected power | 2 | W |
Instantaneous power is F·v; its integral is selected-interaction work.
Negative power removes mechanical energy through this interaction, even if other interactions supply more. Average power is work/duration, not generally endpoint power. This imposed path does not assert the selected force is the net force.
Derive before checking. Retain contrasting captures and explain one assumption that could fail; calculated evidence is not actual laboratory work.
Instantaneous power is F·v; its integral is selected-interaction work.
Negative power removes mechanical energy through this interaction, even if other interactions supply more. Average power is work/duration, not generally endpoint power. This imposed path does not assert the selected force is the net force.
Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.
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Public practice checks a specific claim. It does not establish independent mastery.
Why is a constant-power model singular at a zero-speed start?
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