Derive elastic energy from a force-area construction
Loading an ideal spring slowly from equilibrium requires an external holding force whose magnitude rises from 0 to kx. The force-versus-extension region is a triangle. Its area is½×x×kx=½kx², the stored elastic potential energy when zero is chosen at equilibrium. The factor½ follows from the increasing force; using final force times displacement would overcount.
Learning outcome: Compare compressions 0.10,0.20 and 0.40 m at fixed spring constant. Record force, stored energy and release speed. Then double stiffness while holding compression fixed. Explain why speed scales with the square root of stiffness rather than stiffness itself.
Starting recap
Review signed force components, graph areas, speed squared and system boundaries. Distinguish an interaction force from an energy store or transfer.
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For k=60 N/m and compression 0.20 m, energy is½×60×0.20²=1.2 J. With mass 1 kg and no losses, speed at equilibrium is√2.4≈1.55 m/s. Initial force magnitude is 12 N. Doubling compression to 0.40 m doubles the force to 24 N while energy quadruples to 4.8 J.
Open the experimentPredict
Will doubling compression double or quadruple the speed at equilibrium? Separate the energy scaling from the square root used for speed.
Experiment
Compare compressions 0.10,0.20 and 0.40 m at fixed spring constant. Record force, stored energy and release speed. Then double stiffness while holding compression fixed. Explain why speed scales with the square root of stiffness rather than stiffness itself.
Derive stored energy from a spring-force area
Worked teaching model · synthetic values · Ideal spring initially compressed by selected magnitude, then released to equilibrium on a frictionless horizontal guide with attached mass 1 kg. No spring mass or losses. Force law is linear over this assigned range.
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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 |
|---|---|---|
| Initial spring potential energy | 1.2 | J |
| Spring work to equilibrium | 1.2 | J |
| Kinetic energy at equilibrium | 1.2 | J |
| Speed at equilibrium | 1.54919 | m/s |
| Force magnitude at initial compression | 12 | N |
Accessible plot coordinates
| position (m) | energy (J) |
|---|---|
| -0.4 | 4.8 |
| -0.35 | 3.675 |
| -0.3 | 2.7 |
| -0.25 | 1.875 |
| -0.2 | 1.2 |
| -0.15 | 0.675 |
| -0.1 | 0.3 |
| -0.05 | 0.075 |
| 0 | 0 |
| 0.05 | 0.075 |
| 0.1 | 0.3 |
| 0.15 | 0.675 |
| 0.2 | 1.2 |
| 0.25 | 1.875 |
| 0.3 | 2.7 |
| 0.35 | 3.675 |
| 0.4 | 4.8 |
Stored spring energy grows with compression squared, while initial force grows linearly.
Integrate by geometry: the restoring-force magnitude grows linearly, so quasistatic loading work is triangular area ½(kx)x. Compression and extension of equal magnitude store the same positive energy. At equilibrium the force is zero but speed can be greatest.
Stored spring energy grows with compression squared, while initial force grows linearly.
Integrate by geometry: the restoring-force magnitude grows linearly, so quasistatic loading work is triangular area ½(kx)x. Compression and extension of equal magnitude store the same positive energy. At equilibrium the force is zero but speed can be greatest.
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What changed measurement would reveal energy loss while leaving a static spring-force calibration nearly unchanged?
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