Any general motion of two coupled oscillators can be written as a superposition of the two normal modes (symmetric and antisymmetric). A particularly instructive choice of initial conditions is the “gymnastic” one: displace only one mass and keep the other still.

In this case the resulting motion is a beat. Since the initial state contains both modes in equal measure, and the two modes have slightly different frequencies (ω+\omega_+ and ω\omega_-), they slowly drift out of phase and then back into phase. The observable result is that energy oscillates periodically between the two masses: first only the first one oscillates, then the energy “migrates” to the second, then returns to the first, and so on. The period of this migration is

Tb=2πωω+T_b = \frac{2\pi}{\omega_- - \omega_+}

which is longer the weaker the coupling (i.e. the closer ω\omega_- and ω+\omega_+ are).

Beats in a sentence

Two normal modes of nearby frequencies, superposed, produce a slow back-and-forth of energy. It is the same phenomenon heard as a “beat” when two nearly tuned strings sound together: here, though, the beat is spatial, the energy bounces between the two oscillators.

A classic laboratory example is that of two pendulums coupled by a string: displacing only the first, after a few oscillations the energy passes entirely to the second, then returns. The phenomenon is a prelude to the close energy-level pair of quantum mechanics.

Topics: Oscillations and harmonic motion Concepts: Normal modes · Beats

Related exercises: Problem — Two coupled swings · Worked exercise — Two pendulums coupled by a string · Beats of two nearby frequencies