Periodic motion just means motion that repeats itself in a fixed time interval. A satellite orbiting Earth is periodic. A ball bouncing down a hallway is periodic. A metronome ticking is periodic. All periodic — but not all of them are simple harmonic motion.
That extra rule is what the rest of this lesson is about.
A restoring force is a force exerted in the direction opposite an object's displacement from its equilibrium position. Push a spring's mass to the right, and the spring pulls it left. Pull a pendulum bob to one side, and gravity pulls it back toward center. In both cases, the force's whole job is to undo the displacement.
An equilibrium position is the location at which the net force on an object or system is zero. It's the spot the restoring force is always trying to bring the system back to.
Simple harmonic motion results when the magnitude of the restoring force is proportional to the object's displacement from that equilibrium position:
This is the general SHM condition — it doesn't commit to any particular system. The most familiar system that satisfies it exactly is an ideal spring, where Hooke's law makes the proportionality explicit:
Here k (the spring constant) is just the proportionality constant — a bigger k means a stiffer spring and a stronger restoring force at any given displacement.
Drag the displacement and watch the restoring force respond. Toggle between the spring and the small-angle pendulum — same proportionality, different variable names.
The line is always straight through the origin — that's what "proportional" looks like.
A student pulls a spring-mass system to different displacements and measures the restoring force at each: x = 0.10 m, F = 2.0 N; x = 0.20 m, F = 4.0 N; x = 0.30 m, F = 6.0 N. Show that this system satisfies the SHM condition and find the spring constant k.
A pendulum doesn't obviously look like a spring — there's no x, no k, nothing labeled "Hooke's law." But swing it through a small angle and the same SHM condition reappears, just written in terms of rotation: the restoring torque is proportional to the angular displacement.
Four systems: (1) a block on a spring following Hooke's law F = −kx, (2) a basketball bouncing on a hard floor, (3) a pendulum swinging through a 5° angle, and (4) a child on a swing pushed to a large 60° angle. Which of these exhibit simple harmonic motion?