Use energy to reconstruct speed and turning points
For a horizontal ideal spring, choose spring potential zero at equilibrium. Then U=½kx² and total energy E=½mv²+½kx². At either turning point x=±A, velocity is zero, so E=½kA². In the absence of dissipation or external work, this same total applies at every other position.
Learning outcome: Compare position fractions 0, 0.5 and 1 for one amplitude; reconstruct the total from each pair of energy entries. Then double amplitude while keeping the same position fraction and predict the energy and speed factors before capture.
Starting recap
Review Newton’s second law, radians, sine/cosine graphs, energy and momentum boundaries, and bounded measurement errors.
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Try
For k=20 N/m, m=2 kg and A=0.20 m, E=0.40 J. At x=0.10 m, U=0.10 J and K=0.30 J, giving speed √0.30≈0.548 m/s. Either velocity sign is possible, depending on whether the mass is moving toward or away from the positive endpoint.
Open the experimentPredict
If amplitude doubles, what happens to total mechanical energy and maximum speed?
Experiment
Compare position fractions 0, 0.5 and 1 for one amplitude; reconstruct the total from each pair of energy entries. Then double amplitude while keeping the same position fraction and predict the energy and speed factors before capture.
Partition a constant oscillator energy
Worked teaching model · synthetic values · Horizontal ideal spring k=20 N/m,m=2 kg. U=0 at equilibrium. Position alone gives speed magnitude, not direction; the two possible directions belong to different phases.
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Axes rescale with settings; compare numerical values, not screen angles or apparent lengths. Solid/points show the selected model relationship or observations; the dashed comparison is explained below.
| Quantity | Value | Unit |
|---|---|---|
| Position | 0.1 | m |
| Total mechanical energy | 0.4 | J |
| Spring potential energy | 0.1 | J |
| Kinetic energy | 0.3 | J |
| Speed magnitude | 0.54772 | m/s |
Accessible plot coordinates
| position (m) | energy (J) |
|---|---|
| -0.2 | 0.4 |
| -0.19 | 0.361 |
| -0.18 | 0.324 |
| -0.17 | 0.289 |
| -0.16 | 0.256 |
| -0.15 | 0.225 |
| -0.14 | 0.196 |
| -0.13 | 0.169 |
| -0.12 | 0.144 |
| -0.11 | 0.121 |
| -0.1 | 0.1 |
| -0.09 | 0.081 |
| -0.08 | 0.064 |
| -0.07 | 0.049 |
| -0.06 | 0.036 |
| -0.05 | 0.025 |
| -0.04 | 0.016 |
| -0.03 | 0.009 |
| -0.02 | 0.004 |
| -0.01 | 0.001 |
| 0 | 0 |
| 0.01 | 0.001 |
| 0.02 | 0.004 |
| 0.03 | 0.009 |
| 0.04 | 0.016 |
| 0.05 | 0.025 |
| 0.06 | 0.036 |
| 0.07 | 0.049 |
| 0.08 | 0.064 |
| 0.09 | 0.081 |
| 0.1 | 0.1 |
| 0.11 | 0.121 |
| 0.12 | 0.144 |
| 0.13 | 0.169 |
| 0.14 | 0.196 |
| 0.15 | 0.225 |
| 0.16 | 0.256 |
| 0.17 | 0.289 |
| 0.18 | 0.324 |
| 0.19 | 0.361 |
| 0.2 | 0.4 |
| position (m) | energy (J) |
|---|---|
| -0.2 | 0 |
| -0.19 | 0.039 |
| -0.18 | 0.076 |
| -0.17 | 0.111 |
| -0.16 | 0.144 |
| -0.15 | 0.175 |
| -0.14 | 0.204 |
| -0.13 | 0.231 |
| -0.12 | 0.256 |
| -0.11 | 0.279 |
| -0.1 | 0.3 |
| -0.09 | 0.319 |
| -0.08 | 0.336 |
| -0.07 | 0.351 |
| -0.06 | 0.364 |
| -0.05 | 0.375 |
| -0.04 | 0.384 |
| -0.03 | 0.391 |
| -0.02 | 0.396 |
| -0.01 | 0.399 |
| 0 | 0.4 |
| 0.01 | 0.399 |
| 0.02 | 0.396 |
| 0.03 | 0.391 |
| 0.04 | 0.384 |
| 0.05 | 0.375 |
| 0.06 | 0.364 |
| 0.07 | 0.351 |
| 0.08 | 0.336 |
| 0.09 | 0.319 |
| 0.1 | 0.3 |
| 0.11 | 0.279 |
| 0.12 | 0.256 |
| 0.13 | 0.231 |
| 0.14 | 0.204 |
| 0.15 | 0.175 |
| 0.16 | 0.144 |
| 0.17 | 0.111 |
| 0.18 | 0.076 |
| 0.19 | 0.039 |
| 0.2 | 0 |
Spring and kinetic energy exchange while their sum stays constant.
E=½kA², U=½kx² and K=E−U. Speed follows v²=(k/m)(A²−x²), but its sign requires phase information. These curves are energy against position, not against time.
Spring and kinetic energy exchange while their sum stays constant.
E=½kA², U=½kx² and K=E−U. Speed follows v²=(k/m)(A²−x²), but its sign requires phase information. These curves are energy against position, not against time.
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Why does an energy ledger alone not tell whether the oscillator is approaching a turning point?
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