C.1.5—Mass–spring period

Syllabus
First assessment 2025
Objective
—
Level
HL

Calculate the Period of a Mass–Spring System

Mass–spring period

For an ideal mass mm attached to a linear spring of spring constant kk,

T=2πmkT=2\pi\sqrt{\frac{m}{k}}

Use mm in kilograms and kk in N m−1\mathrm{N\,m^{-1}} to obtain TT in seconds.

Read the dependence

T∝mT\propto\sqrt m: more mass increases the period. T∝1/kT\propto1/\sqrt k: a stiffer spring decreases the period. The ideal period is independent of amplitude while Hooke's law remains valid.

Worked example from local textbook question 6

For T=1.00 sT=1.00\,\mathrm s and k=84 N m−1k=84\,\mathrm{N\,m^{-1}},

m=k(T2π)2=84(1.002π)2=2.13 kgm=k\left(\frac{T}{2\pi}\right)^2=84\left(\frac{1.00}{2\pi}\right)^2=2.13\,\mathrm{kg}

Boundary

This model assumes a linear spring and that the stated oscillating mass includes any effective mass the question requires. Do not substitute amplitude for mm.

C.1.5 Exam Analysis

[ 1 ]

between t=0 and t=T4t=\frac{T}{4};

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.