AP Physics 1 · Unit 7: Oscillations ·  Lesson 7.3

Deep Dive: Representing and Analyzing SHM

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

Two Ways to Write x(t)

An object's displacement in SHM can be represented by either of two equations, and which one you use depends entirely on where you decide t = 0 is:

x(t) = A cos(2πft)
x(t) = A sin(2πft)

Use cosine if the clock starts at the moment of maximum displacement (released from rest at x = +A or x = −A). Use sine if the clock starts at the moment the object passes through equilibrium. Both describe exactly the same kind of motion — they just start the story at a different point in the cycle.

ExampleWorked Example — Choosing Between Cosine and Sine

A block on a spring starts at its equilibrium position and is given a push, so that at t = 0 it has its maximum speed. Which form, x(t) = A cos(2πft) or x(t) = A sin(2πft), correctly represents its displacement — and why?

7.3.A.1.i – 7.3.A.1.iiConcept

Extrema and Zeros — Where Each Variable Peaks

You don't need new formulas to describe velocity and acceleration in SHM — you need to know where each one is at a maximum, a minimum, or zero, and why:

💡Velocity is maximum in magnitude exactly at equilibrium (the object is moving fastest as it passes through the center) and zero exactly at the turning points (the object momentarily stops before reversing direction).
🔑Acceleration is maximum in magnitude exactly at the turning points (where displacement — and therefore the restoring force — is largest) and zero exactly at equilibrium (where the net force is zero, by definition).

Recognizing these positions is what lets you qualitatively describe an entire cycle of motion without ever writing down v(t) or a(t) as formulas.

SynthesisConcept

Why Acceleration and Displacement Are Anti-Phase

This isn't a new fact to memorize — it falls straight out of Lesson 7.1's SHM condition. The restoring force is proportional to −x, and Newton's second law says F = ma, so:

a ∝ −x

Acceleration is always proportional to displacement, with a negative sign built in. Whenever x is at a maximum, a is too — just pointing the opposite way. Whenever x is zero, a is zero. This is what "anti-phase" means: x and a always have opposite sign, everywhere in the cycle. Velocity, meanwhile, is 90° out of step with both — it peaks exactly where they're both zero, and vanishes exactly where they both peak.

Watch the cursor sweep across all three graphs together — one full pass is one period. Notice which graph is at zero exactly when another is at its peak.

Amplitude A (units)1.50
Frequency f (Hz)0.60
x(t)0.00 units
v(t)0.00 units/s
a(t)0.00 units/s²

ExampleGuided Example — Reading the Story from a Graph

A block on a spring starts at t = 0 at its maximum positive displacement (+A), released from rest. Describe the displacement, velocity, and acceleration of the block at t = 0, t = T/4, t = T/2, and t = 3T/4.

Step 1At t = 0 (maximum positive displacement)
x = +A (maximum). v = 0 (a turning point). a is maximum in magnitude, pointing in the negative direction — back toward equilibrium.
7.3.A.2 – 7.3.A.3Concept

Graphical Analysis & Amplitude, Once More

Properties of SHM — period, frequency, phase relationships — can be read directly off graphs of x, v, or a vs. time, without ever writing an equation. This is a skill worth practicing deliberately: given any one of the three graphs, you should be able to sketch the other two by reasoning through the extrema-and-zeros logic from this lesson.

⚠️Changing the amplitude of a system in SHM will not change its period — this was true back in Lesson 7.2, and it's still true here. On a graph, increasing amplitude makes the peaks taller, not the wave wider. If you ever sketch a bigger-amplitude oscillation with a longer or shorter period than the original, something's gone wrong.
← Back to Lesson 7.3Next: Lesson 7.4 →Energy of Simple Harmonic Oscillators — KE and PE trading places every half-cycle.