1. Stationary Waves
Stationary waves
Nodes, antinodes and wavelength
Principle of superposition: when two or more waves meet at a point, the resultant displacement is the sum of the displacements of the individual waves.
A stationary wave forms when two progressive waves of the same frequency (and similar amplitude) travel in opposite directions, usually a wave and its reflection. Drawing the two waves at successive instants and adding them shows points that are always at rest (nodes) and points that oscillate with maximum amplitude (antinodes). Unlike a progressive wave, a stationary wave transfers no energy; all points between adjacent nodes oscillate in phase.
Adjacent nodes (or adjacent antinodes) are λ/2 apart; a node and the nearest antinode are λ/4 apart.
- Stretched string (vibrator at one end, pulley and masses at the other): nodes at both fixed ends; fundamental has L = λ/2.
- Microwaves: a transmitter facing a metal plate; a detector moved along the line finds alternate maxima and minima λ/2 apart.
- Air column: tube closed at one end has a node at the closed end and an antinode at the open end; fundamental L = λ/4. Open at both ends: antinodes at both ends, fundamental L = λ/2 (end corrections ignored).
Stationary waves
node to node = λ/2 node to antinode = λ/4 string with n loops: L = nλ/2
Worked Example
A string 1.20 m long, fixed at both ends, vibrates at 150 Hz with three loops. Find the wavelength and the speed of waves on the string.
Worked Example
A tuning fork of 480 Hz is held over a tube closed at the bottom whose length can be varied. Resonance occurs at lengths of 0.18 m and 0.54 m. Find the speed of sound.
Practice Question
A microwave detector moved between a transmitter and a metal reflector finds successive minima 1.4 cm apart. Find the wavelength and frequency.
2. Diffraction
Diffraction
Spreading through gaps
Diffraction is the spreading of a wave as it passes through a gap or around an edge. The wavelength does not change.
In a ripple tank, plane waves passing through a gap much wider than the wavelength stay nearly straight with only slight spreading at the edges. As the gap is narrowed towards the size of the wavelength the emerging waves become almost circular: diffraction is most noticeable when the gap width is similar to the wavelength.
3. Interference