C.1.6—Simple pendulum period

Syllabus
First assessment 2025
Objective
—
Level
HL

Calculate the Period of a Simple Pendulum

Simple-pendulum period

For a pendulum of length ll undergoing small-angle oscillations,

T=2πlgT=2\pi\sqrt{\frac{l}{g}}

Measure ll from the pivot to the bob's centre of mass and use gg in m s−2\mathrm{m\,s^{-2}}.

Read the dependence

T∝lT\propto\sqrt l and T∝1/gT\propto1/\sqrt g. Bob mass does not appear, so changing mass alone does not change the ideal period.

Worked example from local practice question 9

Changing MM to 4M4M has no effect. Changing ll to 0.25l0.25l gives

T′=2π0.25lg=0.5TT'=2\pi\sqrt{\frac{0.25l}{g}}=0.5T

Boundary

The equation is the small-angle approximation, where sin⁡θ≈θ\sin\theta\approx\theta with θ\theta in radians. Large amplitudes do not follow this period exactly.

C.1.6 Exam Analysis

[ 1 ]

An object performs simple harmonic motion (shm). The graph shows how the velocity v of the object varies with time t.

The displacement of the object is x and its acceleration is a. What is the variation of x with t and the variation of a with t ?

Retrieve the Core C.1 Simple Harmonic Motion Model

Recognize SHM

SHM requires a restoring acceleration a=−ω2xa=-\omega^2x about equilibrium. Track displacement, amplitude, period, frequency and angular frequency with T=1/f=2π/ωT=1/f=2\pi/\omega.

Track one cycle

At an extreme, potential energy is maximum and kinetic energy is zero; at equilibrium, kinetic energy is maximum and potential energy is minimum. Total energy remains constant in ideal SHM.

Read the motion

The gradient of a displacement–time graph is velocity. Acceleration is opposite to displacement. Use the sign of displacement and the gradient to identify direction at any instant.

Final check

Measure displacement from equilibrium, keep amplitude distinct from peak-to-peak distance, and name the relevant potential-energy form for the oscillator.