Interference — Question 6

Section 17-4 · Physics pages 2702–2703

Question 6 Three acoustic contributions can cancel without an opposite pair Three loudspeakers produce equal pressure amplitudes P at a microphone, with received phases 0, 2π/3 and 4π/3. All have the same frequency. Treat source amplitudes as maintained by their drivers. P P P Head-to-tail construction for three received pressure phasors. (a) Find the total pressure phasor. (b) If the third speaker is switched off, find the new amplitude and phase. Why does removing a source increase the measured pressure amplitude?
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Question 6 - Solution Three acoustic contributions can cancel without an opposite pair P P P (a) Method and calculation With the real-part convention, ep = P(1 + e2πi/3 + e4πi/3). Re ep = P(1 −1 2 −1 2) = 0, Im ep = P( √ 3 2 − √ 3 2 ) = 0. The three vectors form a closed triangle. (b) Interpretation and further calculation After removing the third contribution, ep = P(1 + e2πi/3) = P(1 2 + i √ 3 2 ) = Peiπ/3. The resultant amplitude is P with phase π/3. Removing a canceling contribution destroys the null; local acoustic pressure is a coherent sum, not a sum of nonnegative amplitudes. Physical check A local pressure null does not mean the sources emit no sound or that pressure vanishes everywhere.

Question 6

Three acoustic contributions can cancel without an opposite pair

Three loudspeakers produce equal pressure amplitudes PP at a microphone, with received phases 00, 2π/32\pi/3 and 4π/34\pi/3. All have the same frequency. Treat source amplitudes as maintained by their drivers.

Diagram shown in the original SVG worksheet.

  1. Find the total pressure phasor.

  2. If the third speaker is switched off, find the new amplitude and phase. Why does removing a source increase the measured pressure amplitude?

Question 6 - Solution

Three acoustic contributions can cancel without an opposite pair

Diagram shown in the original SVG worksheet.

(a) Method and calculation

With the real-part convention,p̃=P(1+e2πi/3+e4πi/3).\widetilde p=P(1+e^{2\pi i/3}+e^{4\pi i/3}).Re⁡p̃=P(1−12−12)=0,Im⁡p̃=P(32−32)=0.\operatorname{Re}\widetilde p=P(1-\tfrac12-\tfrac12)=0,\quad\operatorname{Im}\widetilde p=P(\tfrac{\sqrt3}2-\tfrac{\sqrt3}2)=0.The three vectors form a closed triangle.

(b) Interpretation and further calculation

After removing the third contribution,p̃=P(1+e2πi/3)=P(12+i32)=Peiπ/3.\widetilde p=P(1+e^{2\pi i/3})=P(\tfrac12+i\tfrac{\sqrt3}2)=Pe^{i\pi/3}.The resultant amplitude is PP with phase π/3\pi/3. Removing a canceling contribution destroys the null; local acoustic pressure is a coherent sum, not a sum of nonnegative amplitudes.

Physical check

A local pressure null does not mean the sources emit no sound or that pressure vanishes everywhere.