All revision notes topics

C.4 Standing waves and resonanceIB Physics SL: Revision notes

Section 1

Formation of standing waves

A standing wave forms when two identical waves (same frequency, wavelength, speed and similar amplitude) travel in opposite directions and superpose, usually a wave and its reflection. The wave profile does not move along; instead each point oscillates with its own amplitude. Unlike a travelling wave, a standing wave has no net transfer of energy along it.

Key termsstanding wavesuperposition

Section 2

Nodes, antinodes, amplitude and phase

Nodes are points of zero amplitude, where the two waves always cancel. Antinodes are points of maximum amplitude. Adjacent nodes (or antinodes) are λ/2 apart; a node and the nearest antinode are λ/4 apart. All points between two adjacent nodes oscillate in phase with different amplitudes; points in neighbouring segments are in antiphase (π rad).

Key termsnodeantinodephase difference
Common mistake

In a standing wave, amplitude varies with position and phase is either 0 or π. In a travelling wave it is the other way round: constant amplitude, phase varying continuously.

Section 3

Strings and pipes

String fixed at both ends: nodes at both ends; L = nλ/2, so fₙ = nv/2L, all harmonics n = 1, 2, 3 …

Pipe open at both ends: displacement antinodes at both ends; also L = nλ/2, all harmonics.

Pipe closed at one end: node at the closed end, antinode at the open end; L = λ/4, 3λ/4, 5λ/4 …, so only odd harmonics (f₁, 3f₁, 5f₁ …) with f₁ = v/4L. For the same length, its fundamental is half that of an open pipe.

Key termsharmonicfirst harmonicclosed pipeopen pipe
Exam tip

Sketch the pattern in words first: count how many quarter- or half-wavelengths fit in L, then use v = fλ.

Section 4

Resonance

Every oscillating system has a natural frequency, the frequency at which it oscillates when displaced and released. A driving (forcing) frequency is imposed by an external periodic force. When the driving frequency equals the natural frequency, resonance occurs: energy is transferred at the greatest rate and the amplitude becomes maximum. The amplitude grows until the energy lost to damping each cycle equals the energy supplied. Far from the natural frequency the amplitude is small.

Key termsnatural frequencydriving frequencyresonance

Section 5

Damping and resonance curves

Damping is the loss of energy from an oscillating system by resistive forces, reducing its amplitude. Increasing damping lowers the maximum amplitude, makes the resonance peak broader (less sharp) and shifts the resonant frequency slightly lower than the natural frequency.

Key termsdampingresonance curve

Section 6

Light, critical and heavy damping

Light (under-) damping: the system oscillates many times with gradually decreasing amplitude (a pendulum in air).

Critical damping: the system returns to equilibrium in the shortest possible time without oscillating (car suspension, door closers).

Heavy (over-) damping: the system returns to equilibrium without oscillating but more slowly than with critical damping (a pendulum in thick oil).

Key termslight dampingcritical dampingheavy damping
Common mistake

Heavy damping does not return a system to equilibrium fastest; critical damping does.

That's the notes covered.

Carry on to the next subtopic.