Part of JWAVE-02 — Waves: Standing Waves, Beats & Doppler Effect

Beats

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Beats arise from superposition of two sound waves with slightly different frequencies f1f_1 and f2f_2. The resultant amplitude modulates at the beat frequency fbeat=f1f2f_{\text{beat}} = |f_1 - f_2|, producing periodic waxing and waning of loudness. Beats are perceptible only when fbeat7f_{\text{beat}} \leq 7 Hz; beyond this, the fluctuations are too rapid for the ear to resolve.

The primary application of beats is determining an unknown frequency. Given a known fork (f1f_1) and beat count (nn), the unknown f2=f1±nf_2 = f_1 \pm n. To resolve the ambiguity: load the unknown fork with wax (decreasing f2f_2). If beats increase, f2f_2 was below f1f_1 (moved further away). If beats decrease, f2f_2 was above f1f_1 (moved closer). Filing the fork increases its frequency — the same logic applies in reverse.

For musical instrument tuning: zero beats between two strings means perfect unison. Piano tuners adjust string tension until beats with a reference fork disappear. In sonometer problems, increasing tension increases wire frequency — combine this with the beat change direction to determine whether the wire was originally above or below the reference frequency.

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