Diffraction by a Circular Aperture — Question 1

Section 36-5 · Physics pages 5932–5933

Question 1 Rayleigh resolution sets a required collecting diameter Two equal incoherent point sources are separated transversely by s = 0.20 m at range R = 20.0 km. An ideal unobstructed circular aperture observes them at λ = 550 nm. Use the Rayleigh criterion θR = 1.22λ/D and small source angles. D focal pattern Schematic; labels, not drawing lengths, specify the data. (a) Find the minimum aperture diameter under this criterion. (b) If the wavelength becomes 825 nm with the same aperture, find the minimum resolvable transverse separation at that range.
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Question 1 - Solution Rayleigh resolution sets a required collecting diameter D focal pattern (a) Method and calculation θs ≃s/R = 1.00 × 10−5 rad; θR ≤θs. Dmin = 1.22λ/θs = 0.0671 m . (b) Interpretation and further calculation sR = R(1.22λ′/D). s′ R = (825/550)(0.20 m) = 0.300 m . Physical check The criterion applies to ideal optics and equal incoherent sources; it is a stated resolution convention rather than a universal detection threshold.

Question 1

Rayleigh resolution sets a required collecting diameter

Two equal incoherent point sources are separated transversely by s=0.20ms=0.20\,\mathrm m at range R=20.0kmR=20.0\,\mathrm{km}. An ideal unobstructed circular aperture observes them at λ=550nm\lambda=550\,\mathrm{nm}. Use the Rayleigh criterion θR=1.22λ/D\theta_R=1.22\lambda/D and small source angles.

Diagram shown in the original SVG worksheet.

  1. Find the minimum aperture diameter under this criterion.

  2. If the wavelength becomes 825nm825\,\mathrm{nm} with the same aperture, find the minimum resolvable transverse separation at that range.

Question 1 - Solution

Rayleigh resolution sets a required collecting diameter

Diagram shown in the original SVG worksheet.

(a) Method and calculation

θs≃s/R=1.00×10−5rad;θR≤θs.\theta_s\simeq s/R=1.00\times10^{-5}\,\mathrm{rad};\quad\theta_R\leq\theta_s.Dmin=1.22λ/θs=0.0671m.\boxed{D_{\min}=1.22\lambda/\theta_s=0.0671\,\mathrm m}.

(b) Interpretation and further calculation

sR=R(1.22λ′/D).s_R=R(1.22\lambda^\prime/D).sR′=(825/550)(0.20m)=0.300m.\boxed{s_R^\prime=(825/550)(0.20\,\mathrm m)=0.300\,\mathrm m}.

Physical check

The criterion applies to ideal optics and equal incoherent sources; it is a stated resolution convention rather than a universal detection threshold.