Construct · 3 fields · 3 citations
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A standing wave is the stationary pattern formed when two waves of the same frequency travel in opposite directions and interfere, giving fixed points of no motion (nodes) and points of maximum motion (antinodes) rather than a travelling disturbance. In acoustics this is how a stretched string or an air column resonates, selecting a discrete set of frequencies (the harmonic series) that give a musical instrument its pitch and timbre. Rayleigh's The Theory of Sound laid out the mathematics of these vibrating systems. The referent is the set of resonant modes of a bounded medium, and it is the same construct that recurs in electromagnetism and quantum mechanics.[1]
The same construct governs electromagnetic fields confined between reflectors or within a cavity: counter-propagating waves interfere to form a standing wave with fixed nodes and antinodes of the field, so only certain wavelengths (the cavity modes) are sustained. Born and Wolf's Principles of Optics develops the interference and resonator theory behind it. It is the identical eigenmode idea as a vibrating string, realised in the electromagnetic field and read from cavity mode wavelengths and the standing-wave ratio rather than from the modes of a string.[2]
In quantum mechanics the same mathematics describes a bound particle: a stationary state is a standing wave of the particle's wavefunction, so confining a particle (as in a particle in a box or an atom) admits only discrete energy levels, the system's quantised eigenstates. Griffiths's Introduction to Quantum Mechanics derives these standing-wave solutions of the Schrödinger equation. It is the same bounded-eigenmode construct as a resonating string or an optical cavity, here realised as matter waves and read from energy levels rather than acoustic frequencies.[3]
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