Conceptly
LessonsFormulasPricing
Sign inStart free
Conceptly
TermsPrivacyRefunds
© 2026 · Physics for everyone
  1. Home
  2. Lessons
  3. Waves
  4. Resonance
All lessons Waves23 min

Resonance

Complete each stage to unlock the next one.

← Standing Waves & ResonanceTemperature and Heat →
01
Hook
02
Explore
03
Formalize
04
Practice
05
Challenge
Interactive simulation
01

Hook

Push a child on a swing and tiny, well-timed nudges build into a soaring arc — but shove at the wrong moment and you just stop them dead. The secret isn't how hard you push, but how often. Aim that same trick at a wine glass or a steel bridge and it can shatter glass or tear metal apart. Why does the timing of a push matter so much more than its strength?

02

Explore

Complete previous stage
03

Formalize

Complete previous stage
04

Practice

Complete previous stage
05

Challenge

Complete previous stage
Spoilers

Resonance — summary and key formula

ShowHide

The question

Push a child on a swing and tiny, well-timed nudges build into a soaring arc — but shove at the wrong moment and you just stop them dead. The secret isn't how hard you push, but how often. Aim that same trick at a wine glass or a steel bridge and it can shatter glass or tear metal apart. Why does the timing of a push matter so much more than its strength?

Every object has a natural frequency at which it vibrates most easily. When a driving force matches that natural frequency, energy builds up dramatically — this is resonance. It is both useful (musical instruments, MRI machines) and dangerous (bridge collapses, earthquake damage).

The key idea

Resonance occurs when a system is driven at its natural (resonant) frequency f_0 = 1/(2π)√(k/m). Energy input is most efficient at this frequency, causing large-amplitude oscillations. Damping limits the maximum amplitude.

Every oscillating system — a spring-mass, a pendulum, a string, a building — has a characteristic natural frequency determined by its stiffness and mass. When driven at f_0, each cycle of the driver synchronises perfectly with the oscillation, so energy accumulates. The Q-factor (quality factor) measures how sharp and strong the resonance is: Q = f_0/(bandwidth). High-Q systems (tuning forks, crystal oscillators) have very sharp resonance peaks and ring for a long time. Low-Q systems (car suspension with shock absorbers) damp quickly. The simulation's damping slider is the damping ratio ζ, the same idea seen from the other side: Q ≈ 1/(2ζ), so a small ζ means a high Q and a tall, narrow peak. With damping present the response actually peaks a touch below f_0, at f_r = f_0·√(1 − 2ζ²) — which is why heavy damping nudges the peak slightly lower as well as flatter. Resonance examples: guitar strings resonate at their fundamental and harmonic frequencies. MRI uses nuclear magnetic resonance. Microwave ovens drive water molecules at their rotational resonance. Engineers must tune building resonant frequencies away from earthquake frequencies.

The formula

f0=12πkmf_0 = \frac{1}{2\pi}\sqrt{\frac{k}{m}}f0​=2π1​mk​​
  • ·f_0 = natural frequency (Hz)
  • ·k = stiffness of restoring force (N/m)
  • ·m = mass of oscillating object (kg)