AP Physics C: Mechanics · Unit 7: Oscillations · Lesson 7.1

Deep Dive: Defining Simple Harmonic Motion

🔬 Deep Dive
This is your textbook for this topic. Take your time. Read it more than once.
7.1.A.1Concept

Periodic Motion and SHM

Welcome to Unit 7. Everything here is about periodic motion — motion that repeats itself at regular intervals: a swinging pendulum, a bouncing ball, a planet orbiting a star, a vibrating guitar string. But this unit zooms in on one particular kind of periodic motion that shows up constantly in physics and engineering: simple harmonic motion (SHM).

🔑Simple harmonic motion is a special case of periodic motion. That means every SHM system is periodic, but not every periodic system is SHM — you'll need a specific test to tell them apart, and that test is exactly what this lesson gives you.

All five of these motions repeat — but only some of them are SHM. Pick one and check whether it passes the restoring-force test.

✓ periodic✓ SHM
The restoring force F = −kΔx is directly proportional to displacement from equilibrium — the textbook case of SHM.

Notice what separates the SHM examples from the non-SHM ones: it isn't just whether the motion repeats. It's about the specific relationship between the force acting on the system and how far that system has moved from where it wants to sit at rest. That relationship is what the next section defines precisely.

7.1.A.27.1.A.2.iMath

The Restoring Force Condition

SHM results when the magnitude of the restoring force exerted on an object is proportional to that object's displacement from its equilibrium position:

F = −kΔx
💡A restoring force is a force exerted in a direction opposite to the object's displacement from equilibrium — that's exactly what the minus sign in F = −kΔx captures. Move the object to the right, and the force pulls left. Move it left, and the force pushes right. It always points back toward equilibrium, never away from it.

Drag the block away from equilibrium and watch the restoring force always point back toward it — growing with distance, per F = −kΔx (here, k = 2 N/m).

Δx (m)3
equilibrium
F = −kΔx = -6.0 NDisplaced right → force points left, back toward equilibrium.

This is the same idea you first saw with an ideal spring back in earlier units — but here it's the definition of the entire category of motion, not just a spring-specific rule. Any system where the restoring force scales linearly with displacement, regardless of what's physically producing that force, exhibits SHM.

7.1.A.2.iiConcept⚠ Watch Out

Equilibrium and Identifying SHM

The restoring force condition only makes sense once you know what it's measured relative to. An equilibrium position is a location at which the net force exerted on an object or system is zero — the spot the system would stay at forever if it were placed there at rest, and the point every restoring force in SHM points back toward.

⚠️Not every force that opposes displacement counts. F = −kΔx requires the force to be directly proportional to displacement — not proportional to displacement squared, not constant, not dependent on velocity instead of position. Any of those variations can still oppose the motion without producing SHM.

Test the SHM condition against five different force (or torque) laws. Only one thing matters: is the restoring force's magnitude directly proportional to displacement?

✓ produces SHM
Matches the SHM condition exactly — force magnitude proportional to displacement, directed opposite to it.

This classifying skill — checking a force or torque law against F = −kΔx before assuming SHM applies — is the foundation for the rest of Unit 7. Once you can confidently identify SHM, every equation for period, frequency, position, velocity, acceleration, and energy in the coming lessons becomes a tool you know exactly when to reach for.

← Back to Lesson 7.1Ready for 7.2? Frequency and Period of SHM puts numbers to the motion you can now recognize.