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SCIENCE · INVESTIGATE AND EXPLAIN

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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Try

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 experiment

Predict

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.

Reset keeps your prediction, captures and practice history.

-0.40.44.80position (m)energy (J)

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.

Calculated evidence ledger — synthetic teaching model
QuantityValueUnit
Initial spring potential energy1.2J
Spring work to equilibrium1.2J
Kinetic energy at equilibrium1.2J
Speed at equilibrium1.54919m/s
Force magnitude at initial compression12N
Accessible plot coordinates
Primary plotted points
position (m)energy (J)
-0.44.8
-0.353.675
-0.32.7
-0.251.875
-0.21.2
-0.150.675
-0.10.3
-0.050.075
00
0.050.075
0.10.3
0.150.675
0.21.2
0.251.875
0.32.7
0.353.675
0.44.8

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.

Captures preserve recipes and replay their calculated results. They are synthetic model evidence, not physical measurements.

Understand

1. Orient: 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.

2. Explain and derive

Equal-magnitude compression and extension store the same positive energy because x is squared. Their restoring forces point in opposite directions. Force depends linearly on signed displacement, while energy depends quadratically on its magnitude. Doubling compression doubles initial force but quadruples stored energy.

For a frictionless horizontal spring–object system released from rest, initial spring energy becomes kinetic energy as the spring reaches equilibrium. Set½kx₀²=½mv² to obtain speed|x₀|√(k/m). The force is zero at equilibrium, yet speed can be maximum there because energy has accumulated during the preceding motion.

The energy relation predicts speed magnitude at a position, not which way the object is moving. Direction requires initial conditions and motion history. The ideal model omits spring mass, internal damping and the elastic limit. A real stiffness inferred at small extension should not be extrapolated to a large stretch without evidence.

3. Work an example

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.

4. Predict and investigate

Predict first: Will doubling compression double or quadruple the speed at equilibrium? Separate the energy scaling from the square root used for speed.

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. Use the lesson controls and retain the settings with your evidence.

5. Transfer and explain

Try a new practice case

A spring with k=80 N/m is compressed by 0.10 m. Find its stored elastic potential energy.

This extra practice is not saved and does not award mastery. Record your first answer, explanation and whether you revealed help in the lesson notebook. Use the lesson’s saved question separately.

6. Reflect and retain evidence

What changed measurement would reveal energy loss while leaving a static spring-force calibration nearly unchanged?

Retain a first attempt, signed ledger, units, system boundary, assumptions and a changed-case prediction. Public worked checks are practice, not independent mastery evidence. Synthetic outputs are not physical measurements.

Framework and source notes

Original teaching prose and numerical cases. College Board AP Physics 1 CED, Unit 3 topic mapping: 3.3; 3.4. Checked 30 October 2026; this is a content cross-reference, not AP authorization.

Apply

An ideal spring with k=100 N/m is compressed by 0.20 m. How much elastic energy is stored?

Public practice checks a specific claim. It does not establish independent mastery.

What changed measurement would reveal energy loss while leaving a static spring-force calibration nearly unchanged?

Continue

Completion requires a saved prediction, at least one capture and a reflection. Presence checks do not grade your reasoning.

Skipping retains experiments and awards no mastery.

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