Interference — Question 7

Section 17-4 · Physics pages 2704–2705

Question 7 Phase jitter washes out a designed interference minimum At a microphone two equal-amplitude tones have pressure amplitudes P and relative phase π + ϵ. The phase error is slowly and uniformly distributed over [−a, a]. Average first over carrier cycles and then over phase error. |ϵ| ⟨p2⟩ Residual mean-square pressure grows away from the ideal cancellation phase. (a) Derive the averaged mean-square pressure as a function of a. (b) For a = π/2, compare the result with the sum of the two separate mean-square pressures. State the small-a limit.
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Question 7 - Solution Phase jitter washes out a designed interference minimum |ϵ| ⟨p2⟩ (a) Method and calculation For fixed error, the combined mean-square pressure is ⟨p2⟩cycle = P 2[1 + cos(π + ϵ)] = P 2(1 −cos ϵ). Uniform phase averaging gives ⟨p2⟩= P 2 [ 1 −1 2a ∫a −a cos ϵ dϵ ] = P 2 ( 1 −sin a a ) . (b) Interpretation and further calculation The separate mean-square pressures sum to P 2. At a = π/2, the ratio is 1 −2 π = 0.36338. For small a, sin a/a = 1 −a2/6 + O(a4), so the residual is P 2a2/6. The null degrades quadratically with small uniformly distributed phase error. Physical check The averaging convention matters: P is a peak pressure amplitude, so each isolated sinusoid has mean square P 2/2.

Question 7

Phase jitter washes out a designed interference minimum

At a microphone two equal-amplitude tones have pressure amplitudes PP and relative phase π+ϵ\pi+\epsilon. The phase error is slowly and uniformly distributed over [−a,a][-a,a]. Average first over carrier cycles and then over phase error.

Diagram shown in the original SVG worksheet.

  1. Derive the averaged mean-square pressure as a function of aa.

  2. For a=π/2a=\pi/2, compare the result with the sum of the two separate mean-square pressures. State the small-aa limit.

Question 7 - Solution

Phase jitter washes out a designed interference minimum

Diagram shown in the original SVG worksheet.

(a) Method and calculation

For fixed error, the combined mean-square pressure is⟨p2⟩cycle=P2[1+cos⁡(π+ϵ)]=P2(1−cos⁡ϵ).\langle p^2\rangle_{\mathrm{cycle}}=P^2[1+\cos(\pi+\epsilon)]=P^2(1-\cos\epsilon).Uniform phase averaging gives⟨p2⟩¯=P2[1−12a∫−aacosϵdϵ]=P2(1−sin⁡aa).\overline{\langle p^2\rangle}=P^2\left[1-\frac1{2a}\int_{-a}^a\cos\epsilon\,d\epsilon\right]=P^2\left(1-\frac{\sin a}{a}\right).

(b) Interpretation and further calculation

The separate mean-square pressures sum to P2P^2. At a=π/2a=\pi/2, the ratio is1−2π=0.36338.1-\frac2\pi=0.36338.For small aa, sin⁡a/a=1−a2/6+O(a4)\sin a/a=1-a^2/6+O(a^4), so the residual is P2a2/6P^2a^2/6. The null degrades quadratically with small uniformly distributed phase error.

Physical check

The averaging convention matters: PP is a peak pressure amplitude, so each isolated sinusoid has mean square P2/2P^2/2.