Academy
PhysicsOscillationsShmThe Simple Pendulum

The Simple Pendulum

SHM approximation for small angles — why a pendulum swings isochronously and how length determines period.

A pendulum is not strictly SHM. But for small angles — less than about 15° — it is a near-perfect approximation. This is one of the most elegant results in physics.

The motion

Bob swings in an arc. The restoring force is the component of gravity tangential to the arc:

F=mgsinθmgθ(for small θ)F = -mg\sin\theta \approx -mg\theta \quad \text{(for small } \theta\text{)}

This linear approximation makes it SHM. The angular frequency is:

ω=gL,T=2πLg\omega = \sqrt{\frac{g}{L}}, \quad T = 2\pi\sqrt{\frac{L}{g}}

Pendulum length 150 angle 15
Show string bob pivot arc graph-x energy KE PE E
Hide readouts angle-label

Watch the θ(t) graph — a perfect cosine. KE and PE exchange continuously just as in the spring-mass system.

Period depends on length, not mass

The mass cancels completely in the derivation. A heavy bob and a light bob on the same string swing identically.

Short pendulum (LL small, faster):

Pendulum length 80 angle 15
Show string bob pivot arc graph-x readouts
Hide energy angle-label

Long pendulum (LL large, slower):

Pendulum length 200 angle 15
Show string bob pivot arc graph-x readouts
Hide energy angle-label

Both start at the same 15° angle. The longer pendulum takes more time per cycle. T displayed in the readout — longer string, longer period.

TLT \propto \sqrt{L}

Doubling the length increases the period by 21.41\sqrt{2} \approx 1.41.

Period is independent of amplitude (for small angles)

Pull the bob to 10° or 20° — the period barely changes. This is the isochronous property again, now in a pendulum:

Pendulum length 150 angle 8
Snapshot at extreme
Show string bob pivot arc
Hide graph-x energy readouts
Pendulum length 150 angle 25
Snapshot at extreme
Show string bob pivot arc
Hide graph-x energy readouts

Same length, different angles. Period is approximately the same for both — as long as the angle stays small.

For large angles, the sinθθ\sin\theta \approx \theta approximation breaks down and the period increases. At 90° the error is about 18%.

At the extremes — maximum PE, zero KE

Bob momentarily at rest at maximum angle. All energy is gravitational PE:

Pendulum length 150 angle 20
Snapshot at extreme
Show string bob pivot arc energy KE PE E
Hide graph-x readouts angle-label

At the centre — maximum KE, zero PE

Bob passes through lowest point at maximum speed. All energy is kinetic:

Pendulum length 150 angle 20
Snapshot at centre
Show string bob pivot arc energy KE PE E
Hide graph-x readouts angle-label

Effect of gravity

On the Moon (g=1.6g = 1.6 m/s²), the same pendulum swings much slower:

Pendulum length 150 angle 15 g 9.8
Show string bob pivot readouts
Hide graph-x energy angle-label arc
Pendulum length 150 angle 15 g 1.6
Show string bob pivot readouts
Hide graph-x energy angle-label arc

Period on Moon is 9.8/1.62.47\sqrt{9.8/1.6} \approx 2.47 times longer than on Earth.

Key results

ω=gL,T=2πLg,f=12πgL\omega = \sqrt{\frac{g}{L}}, \quad T = 2\pi\sqrt{\frac{L}{g}}, \quad f = \frac{1}{2\pi}\sqrt{\frac{g}{L}}

  • TT depends on LL and gg only — not mass, not amplitude (for small angles)
  • TLT \propto \sqrt{L} — double length → period ×2\times\sqrt{2}
  • T1/gT \propto 1/\sqrt{g} — weaker gravity → longer period