Diffraction by a Circular Aperture — Question 10

Section 36-5 · Physics pages 5950–5951

Question 10 Diffraction and aperture-dependent aberration can favor a finite opening In a supplied engineering model, total angular blur is θ2 tot = (A/D)2 + (BD2)2, with A = 1.22λ, λ = 500 nm, and B = 0.0100 m−2. The two blur contributions add in quadrature; this is an approximate model. D θ Schematic; labels, not drawing lengths, specify the data. (a) Derive the aperture diameter minimizing the total blur. (b) Evaluate the optimum diameter and minimum blur, and find the ratio of diffraction blur to aberration blur there.
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Question 10 - Solution Diffraction and aperture-dependent aberration can favor a finite opening D θ (a) Method and calculation dθ2 tot dD = −2A2 D3 + 4B2D3 = 0 =⇒D6 = A2/(2B2). Dopt = ( A √ 2B )1/3 = 35.0702 mm . (b) Interpretation and further calculation θd = 17.3937 µrad, θa = 12.2992 µrad, θmin = 21.3028 µrad . A2/D2 = 2B2D4 =⇒θd/θa = √ 2 . Physical check The optimum does not occur at equal blur contributions because the two terms have different powers of aperture diameter.

Question 10

Diffraction and aperture-dependent aberration can favor a finite opening

In a supplied engineering model, total angular blur is θtot2=(A/D)2+(BD2)2\theta_{\mathrm{tot}}^2=(A/D)^2+(BD^2)^2, with A=1.22λA=1.22\lambda, λ=500nm\lambda=500\,\mathrm{nm}, and B=0.0100m−2B=0.0100\,\mathrm{m^{-2}}. The two blur contributions add in quadrature; this is an approximate model.

Diagram shown in the original SVG worksheet.

  1. Derive the aperture diameter minimizing the total blur.

  2. Evaluate the optimum diameter and minimum blur, and find the ratio of diffraction blur to aberration blur there.

Question 10 - Solution

Diffraction and aperture-dependent aberration can favor a finite opening

Diagram shown in the original SVG worksheet.

(a) Method and calculation

dθtot2dD=−2A2D3+4B2D3=0⇒D6=A2/(2B2).\frac{d\theta_{\mathrm{tot}}^2}{dD}=-\frac{2A^2}{D^3}+4B^2D^3=0\Longrightarrow D^6=A^2/(2B^2).Dopt=(A2B)1/3=35.0702mm.\boxed{D_{\mathrm{opt}}=\left(\frac A{\sqrt2B}\right)^{1/3}=35.0702\,\mathrm{mm}}.

(b) Interpretation and further calculation

θd=17.3937μrad,θa=12.2992μrad,θmin=21.3028μrad.\boxed{\theta_d=17.3937\,\mu\mathrm{rad},\quad\theta_a=12.2992\,\mu\mathrm{rad},\quad\theta_{\min}=21.3028\,\mu\mathrm{rad}}.A2/D2=2B2D4⇒θd/θa=2.A^2/D^2=2B^2D^4\Longrightarrow\boxed{\theta_d/\theta_a=\sqrt2}.

Physical check

The optimum does not occur at equal blur contributions because the two terms have different powers of aperture diameter.