186, 188–191OscillationsStretch

Damping and Resonance

Push a child on a swing at just the right moment each time and a small effort builds a large swing. Push at the wrong rhythm and nothing much happens. That is resonance\textbf{resonance} — and it can shatter a wine glass, collapse a bridge or, used well, tune a radio.

35 min Topic 13 · Oscillations

What you'll be able to do

  • Distinguish free and forced oscillations
  • Describe light, critical and heavy damping and their effects
  • Explain resonance and sketch amplitude–frequency response curves
  • Describe applications and problems of resonance
1

Free and forced oscillations

A free oscillation\textbf{free oscillation} occurs when a system is displaced and released with no further external force. It vibrates at its natural frequency\textbf{natural frequency} f0f_{0}, determined by its properties — such as mm and kk for a spring.

A forced oscillation\textbf{forced oscillation} occurs when a periodic external force drives the system. After an initial settling period, it oscillates at the driving frequency\textbf{driving frequency}, not its natural frequency.

The amplitude of a forced oscillation depends on how close the driving frequency is to the natural frequency, and on the damping.

2

Damping

Damping\textbf{Damping} is the loss of energy from an oscillating system caused by resistive forces such as air resistance or friction. The energy is usually transferred to thermal energy in the surroundings. It reduces the amplitude over time.

Light damping\textbf{Light damping}: the amplitude decreases gradually over many oscillations, with the period almost unchanged. A pendulum in air is lightly damped.

Critical damping\textbf{Critical damping}: the system returns to equilibrium in the shortest possible time without oscillating. Car suspension is designed to be close to critically damped.

Heavy damping\textbf{Heavy damping} (overdamping): the system returns to equilibrium without oscillating, but more slowly than with critical damping — like a pendulum moving through thick oil.

Example 1A lightly damped oscillator loses 10% of its amplitude each cycle. What fraction of its original energy remains after 3 cycles?
1Amplitude after 3 cycles: 0.903=0.7290.90^{3} = 0.729 of original.
2Energy ∝A2\propto A^{2}: 0.72920.729^{2}.
AnswerAbout 0.530.53 — just over half the energy.

Tip — For light damping, amplitude decays exponentially: each cycle loses the same fraction\textit{fraction}, not the same amount.

3

Resonance

Resonance\textbf{Resonance} occurs when the driving frequency equals the natural frequency of the system. Energy is then transferred from the driver to the oscillator most efficiently, and the amplitude reaches a maximum.

At resonance, the driver and oscillator are in step so that every push adds energy — the driving force is in phase with the velocity.

A graph of amplitude against driving frequency peaks at the natural frequency. With less damping\textbf{less damping} the peak is taller and narrower. With more damping\textbf{more damping} it is lower and broader, and the peak shifts slightly below f0f_{0}.

With no damping at all, the amplitude would grow without limit; in practice something breaks or damping always intervenes.

4

Resonance in practice

Useful\textbf{Useful}: musical instruments use resonance in air columns and strings to amplify particular notes; radios are tuned by adjusting a circuit’s natural frequency to match a station; MRI scanners use resonance of hydrogen nuclei in a strong magnetic field.

Harmful\textbf{Harmful}: bridges and buildings can resonate with wind or footsteps. London’s Millennium Bridge swayed when pedestrians fell into step with its sideways motion and had to be fitted with dampers. Tall buildings in earthquake zones use tuned mass dampers to absorb energy at their natural frequency.

Engineers avoid harmful resonance by changing a structure’s natural frequency away from likely driving frequencies, or by adding damping to flatten the response.

Tip — In "suggest how" questions about resonance problems, give one of: change natural frequency (mass or stiffness), or increase damping.

Equation recap

fresonance≈f0f_{\text{resonance}} \approx f_{0}
Resonance condition.
f0=12πkmf_{0} = \dfrac{1}{2\pi}\sqrt{\dfrac{k}{m}}
Natural frequency of a spring.
E∝A2E \propto A^{2}
Energy and amplitude.

Common mistakes to avoid

Saying a forced oscillator vibrates at its natural frequency.
It vibrates at the driving frequency.
Saying damping changes the natural frequency greatly.
Light damping barely changes the frequency; it reduces amplitude.
Saying heavy damping returns fastest.
Critical damping returns fastest without oscillating.
Drawing a more damped curve with a taller peak.
More damping gives a lower, broader peak.

Key takeaways

  • Free oscillations are at the natural frequency; forced oscillations are at the driving frequency.
  • Damping transfers energy away and reduces amplitude.
  • Light damping: slow decay. Critical: fastest return without oscillation. Heavy: slow return.
  • Resonance: driving frequency equals natural frequency, giving maximum amplitude.
  • More damping gives a lower, broader resonance peak.

Test yourself

Answer a few questions, then review anything you missed.

Next step

Keep practising

Start with the quiz above to check the key ideas. You can also choose another topic from the practice library.

Browse practice topics

Related lessons

All 4 lessons