C.1.5—Mass–spring period
- Syllabus
- First assessment 2025
- Objective
- —
- Level
- HL
Mass–spring period
For an ideal mass m attached to a linear spring of spring constant k,
T=2πkm
Use m in kilograms and k in Nm−1 to obtain T in seconds.
Read the dependence
T∝m: more mass increases the period. T∝1/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=1.00s and k=84Nm−1,
m=k(2πT)2=84(2π1.00)2=2.13kg
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 m.
[ 1 ]
between t=0 and t=4T;
Recognize SHM
SHM requires a restoring acceleration a=−ω2x about equilibrium. Track displacement, amplitude, period, frequency and angular frequency with T=1/f=2π/ω.
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.