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SCIENCE · INVESTIGATE AND EXPLAIN

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.

All lessons are open directly. Your saved experiments remain when you leave and return.

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 experiment

Predict

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.

Reset keeps your prediction, captures and practice history.

-0.20.20.40position (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
Position0.1m
Total mechanical energy0.4J
Spring potential energy0.1J
Kinetic energy0.3J
Speed magnitude0.54772m/s
Accessible plot coordinates
Primary plotted points
position (m)energy (J)
-0.20.4
-0.190.361
-0.180.324
-0.170.289
-0.160.256
-0.150.225
-0.140.196
-0.130.169
-0.120.144
-0.110.121
-0.10.1
-0.090.081
-0.080.064
-0.070.049
-0.060.036
-0.050.025
-0.040.016
-0.030.009
-0.020.004
-0.010.001
00
0.010.001
0.020.004
0.030.009
0.040.016
0.050.025
0.060.036
0.070.049
0.080.064
0.090.081
0.10.1
0.110.121
0.120.144
0.130.169
0.140.196
0.150.225
0.160.256
0.170.289
0.180.324
0.190.361
0.20.4
Dashed comparison coordinates
position (m)energy (J)
-0.20
-0.190.039
-0.180.076
-0.170.111
-0.160.144
-0.150.175
-0.140.204
-0.130.231
-0.120.256
-0.110.279
-0.10.3
-0.090.319
-0.080.336
-0.070.351
-0.060.364
-0.050.375
-0.040.384
-0.030.391
-0.020.396
-0.010.399
00.4
0.010.399
0.020.396
0.030.391
0.040.384
0.050.375
0.060.364
0.070.351
0.080.336
0.090.319
0.10.3
0.110.279
0.120.256
0.130.231
0.140.204
0.150.175
0.160.144
0.170.111
0.180.076
0.190.039
0.20

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.

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

Understand

1. Frame the question

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.

2. Build the mechanism

Subtracting potential from total gives K=½k(A²−x²) and v²=(k/m)(A²−x²). This determines speed magnitude, not signed velocity. The allowed positions satisfy |x|≤A; asking for a real speed outside that range contradicts the assigned energy rather than revealing a negative kinetic energy.

At equilibrium all this mechanical energy is kinetic and speed is greatest. At the endpoints it is all potential. At x=A/2, potential is one-quarter of total and kinetic is three-quarters: energy depends on displacement squared, so halfway in position is not halfway in energy. Equal energy shares occur at |x|=A/√2.

A potential-energy-versus-position graph is an upward parabola. The fixed total-energy line intersects it at the two turning points, and their vertical separation gives kinetic energy. This is not a time graph: the oscillator spends more time near turning points where it moves slowly. For a vertical spring the shifted effective potential must include gravity consistently rather than dropping gravitational energy silently.

3. Work an example

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.

4. Predict and investigate

If amplitude doubles, what happens to total mechanical energy and maximum speed?

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.

5. Transfer to a new case

Try a new practice case

A spring has k=50 N/m and amplitude 0.4 m. Find its total mechanical 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. Explain the boundary

Why does an energy ledger alone not tell whether the oscillator is approaching a turning point?

These are bounded virtual models and supplied numerical cases, not independent measurements or an observed physical investigation. Do not construct spring, pendulum or collision apparatus from these instructions. Practical evidence requires an appropriate supervised setting.

Sources

Original explanations, worked cases and numerical models. Framework checked 30 October 2026: AP Physics 1 Course and Exam Description, topics 7.4. Mechanism reference: OpenStax University Physics 1, simple harmonic motion and pendulums. No official assessment items reproduced.

Apply

At x=A/2 in an ideal spring oscillator, the kinetic-energy fraction is:

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

Why does an energy ledger alone not tell whether the oscillator is approaching a turning point?

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