Interference of Waves — Question 7

Section 16-9 · Physics pages 2564–2565

Question 7 Random relative phase removes the coherent cross term on average Two equal-amplitude waves have instantaneous phase difference ∆. During a long measurement, ∆samples the interval [0, 2π) uniformly, slowly compared with the oscillation period. Each wave alone carries mean power P0. Re Im A1 A2 A3 A4 Possible relative phase orientations across repeated measurements; the arrows depict alternatives, not four simultaneous waves. (a) Find the long-time averaged total power. (b) Compare with a permanently fixed phase difference π/2. Can a single averaged power reading distinguish these two situations?
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Question 7 - Solution Random relative phase removes the coherent cross term on average Re Im A1 A2 A3 A4 Method and mathematical working Average the interference term over the phase distribution. Uniform phase over a complete cycle has zero mean cosine, even though each realization can interfere strongly. ⟨cos ϕ⟩= 1 2π ∫2π 0 cos ϕ dϕ = 0, ⟨P⟩= 2P 0. ⟨P⟩= 2P0[1 + ⟨cos ϕ⟩] = 2P0, ϕ = π/2 ⇒P = 2P0 in every realization. (a) Calculation and conclusion At fixed relative phase, cycle-averaged power is 2P0(1 + cos ∆). Uniform phase averaging gives ⟨cos ∆⟩= 0, hence ⟨P⟩= 2P0. (b) Interpretation and limits At fixed quadrature, cos(π/2) = 0, so the same power 2P0 results. But the coherent quadrature sum has a stable phase and amplitude, whereas the random-phase sum fluctuates. A single mean-power reading cannot establish coherence; phase-sensitive or time-resolved observations are needed. Physical check A fixed quadrature phase gives the same mean power but no phase-induced variation from trial to trial. The mean alone cannot distinguish these two statistical situations.

Question 7

Random relative phase removes the coherent cross term on average

Two equal-amplitude waves have instantaneous phase difference Δ\Delta. During a long measurement, Δ\Delta samples the interval [0,2π)[0,2\pi) uniformly, slowly compared with the oscillation period. Each wave alone carries mean power P0P_0.

Diagram shown in the original SVG worksheet.

  1. Find the long-time averaged total power.

  2. Compare with a permanently fixed phase difference π/2\pi/2. Can a single averaged power reading distinguish these two situations?

Question 7 - Solution

Random relative phase removes the coherent cross term on average

Diagram shown in the original SVG worksheet.

Method and mathematical working

Average the interference term over the phase distribution. Uniform phase over a complete cycle has zero mean cosine, even though each realization can interfere strongly.⟨cos⁡ϕ⟩=12π∫02πcos⁡ϕdϕ=0,⟨P¯⟩=2P¯0.⟨P¯⟩=2P0[1+⟨cos⁡ϕ⟩]=2P0,ϕ=π/2⇒P¯=2P0in every realization.\begin{aligned}\langle\cos\phi\rangle&=\frac1{2\pi}\int_0^{2\pi}\cos\phi\,d\phi=0,\\\langle\overline P\rangle&=2\overline P_0.\\[4pt]\langle\overline P\rangle&=2P_0[1+\langle\cos\phi\rangle]=2P_0,\\\phi=\pi/2&\Rightarrow\overline P=2P_0\quad\text{in every realization}.\end{aligned}

(a) Calculation and conclusion

At fixed relative phase, cycle-averaged power is 2P0(1+cos⁡Δ)2P_0(1+\cos\Delta). Uniform phase averaging gives ⟨cos⁡Δ⟩=0\langle\cos\Delta\rangle=0, hence ⟨P⟩=2P0\langle P\rangle=2P_0.

(b) Interpretation and limits

At fixed quadrature, cos⁡(π/2)=0\cos(\pi/2)=0, so the same power 2P02P_0 results. But the coherent quadrature sum has a stable phase and amplitude, whereas the random-phase sum fluctuates. A single mean-power reading cannot establish coherence; phase-sensitive or time-resolved observations are needed.

Physical check

A fixed quadrature phase gives the same mean power but no phase-induced variation from trial to trial. The mean alone cannot distinguish these two statistical situations.