Coherence — Question 3

Section 35-4 · Physics pages 5776–5777

Question 3 A finite exposure can average a slowly moving fringe to zero contrast Two equal beams have a frequency difference ∆ν. After averaging over the optical carrier, their intensity is I(t) = 2I0[1 + cos(δ + 2π∆νt)]. A rectangular exposure extends from −T/2 to T/2. Define sinc x = sin x/x. t I exposure T Schematic; labels, not drawing lengths, specify the data. (a) Integrate the recorded intensity and derive the exposure-limited visibility. (b) For ∆ν = 100 Hz, find the first positive exposure duration with zero visibility and the visibility for T = 5.0 ms.
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Question 3 - Solution A finite exposure can average a slowly moving fringe to zero contrast t I exposure T (a) Method and calculation I = 1 T ∫T/2 −T/2 I(t)dt = 2I0 [ 1 + sin(π∆νT) π∆νT cos δ ] . V = | sinc(π∆νT)| . (b) Interpretation and further calculation π∆νT = π =⇒Tzero = 1/∆ν = 10.0 ms . T = 5.0 ms : V = sin(π/2)/(π/2) = 2/π = 0.63662 . Physical check Instantaneous interference can be strong even when an integrating detector records no stationary fringe contrast.

Question 3

A finite exposure can average a slowly moving fringe to zero contrast

Two equal beams have a frequency difference Δν\Delta\nu. After averaging over the optical carrier, their intensity is I(t)=2I0[1+cos⁡(δ+2πΔνt)]I(t)=2I_0[1+\cos(\delta+2\pi\Delta\nu t)]. A rectangular exposure extends from −T/2-T/2 to T/2T/2. Define sinc⁡x=sin⁡x/x\operatorname{sinc}x=\sin x/x.

Diagram shown in the original SVG worksheet.

  1. Integrate the recorded intensity and derive the exposure-limited visibility.

  2. For Δν=100Hz\Delta\nu=100\,\mathrm{Hz}, find the first positive exposure duration with zero visibility and the visibility for T=5.0msT=5.0\,\mathrm{ms}.

Question 3 - Solution

A finite exposure can average a slowly moving fringe to zero contrast

Diagram shown in the original SVG worksheet.

(a) Method and calculation

I¯=1T∫−T/2T/2I(t)dt=2I0[1+sin⁡(πΔνT)πΔνTcosδ].\overline I=\frac1T\int_{-T/2}^{T/2}I(t)dt=2I_0\left[1+\frac{\sin(\pi\Delta\nu T)}{\pi\Delta\nu T}\cos\delta\right].V=|sinc⁡(πΔνT)|.\boxed{V=|\operatorname{sinc}(\pi\Delta\nu T)|}.

(b) Interpretation and further calculation

πΔνT=π⇒Tzero=1/Δν=10.0ms.\pi\Delta\nu T=\pi\Longrightarrow\boxed{T_{\mathrm{zero}}=1/\Delta\nu=10.0\,\mathrm{ms}}.T=5.0ms:V=sin⁡(π/2)/(π/2)=2/π=0.63662.T=5.0\,\mathrm{ms}:\quad\boxed{V=\sin(\pi/2)/(\pi/2)=2/\pi=0.63662}.

Physical check

Instantaneous interference can be strong even when an integrating detector records no stationary fringe contrast.