Conditions for SHM
An oscillator moves with SHM only if all three hold:
- Acceleration is directed towards a fixed equilibrium point.
- Acceleration is in the opposite direction to displacement.
- Acceleration is directly proportional to displacement from that point.
a–x graph: straight line through the origin, gradient = −ω².
Whenever displacement is positive, acceleration is negative (and vice versa) — always directly proportional, never a curve.
x, v, a — how they relate
v–t is the gradient of x–t; a–t is the gradient of v–t.
- At maximum displacement (x=±A): v=0, a is maximum (opposite direction).
- At equilibrium (x=0): v is maximum (v_max=ωA), a=0.
Link to circular motion
SHM = the projection of circular motion onto a diameter.
Picture a particle spinning at radius r; its shadow on a diameter oscillates with SHM. This gives x = A cos θ = A cos ωt, where:
| Circular motion | SHM |
| Radius, r | Amplitude, A |
| Angular displacement, θ | Phase, ωt |
| Angular velocity, ω | Angular frequency, ω |
Key definitions
- Amplitude, A — maximum displacement from equilibrium (m).
- Period, T — time for one complete cycle (s).
- Frequency, f — complete oscillations per second (Hz).
- Phase — position within a cycle; phase difference = 2πΔt/T = ωΔt (rad).
In phase / antiphase: a phase difference of a multiple of 2π rad means back in phase; π rad means exactly out of phase (antiphase).