Oppositely phased resonators short-circuit each other and prolong sound decay.

Evidence

Three of the four cases mentioned here are illustrated in figure 13.7. Starting with the same pressure in both resonators, there is a resonant addition of amplitudes resulting in louder sound. Since the sound is louder, the energy is drained faster from the resonators (figure 13.7, left). For in-phase oscillation of the resonators, their amplitudes add, giving approximately twice the amplitude far away, and thus instead of twice the power, we get four times the power of a single resonator. This means a doubling of the rate of energy dumping per resonator—that is, exponential decay with an exponent that is twice as large, and a Q half as large (see section 10.3). Indeed, from the figure we see this faster decay and an estimate gives a Q of 9 for the in-phase case as compared to 18 for the single oscillator. — Eric J. Heller, Why You Hear What You Hear- An…, 1233 (#expands, via linked claim)

Categorization

  • XREF: connects to: Adjacent compression and rarefaction regions can short-circuit and kill radiated sound; Marimba resonators amplify sound by capturing near-field energy that would otherwise short-circuit; In-phase coupled resonators radiate four times the power of one resonator. — Eric J. Heller, Why You Hear What You Hear- An…, 1233

Broader Connections