Diffraction by a Circular Aperture — Question 6

Section 36-5 · Physics pages 5942–5943

Question 6 The Bessel expansion gives the curvature of the central Airy peak For a circular aperture, I/Ic = [2J1(u)/u]2 with u = πD sin θ/λ. Use J1(u) = u/2 −u3/16 + u5/384 + O(u7). Let D = 10.0 mm and λ = 500 nm. u I/Ic Schematic; labels, not drawing lengths, specify the data. (a) Derive the central intensity expansion through fourth order. (b) Use its quadratic term to estimate the angle causing a one-percent drop from the peak, and compare with the Rayleigh angle.
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Question 6 - Solution The Bessel expansion gives the curvature of the central Airy peak u I/Ic (a) Method and calculation 2J1(u)/u = 1 −u2/8 + u4/192 + O(u6). I/Ic = 1 −u2/4 + 5u4/192 + O(u6) . (b) Interpretation and further calculation u2/4 = 0.01 =⇒u = 0.20 =⇒θ ≃0.20λ/(πD) = 3.18310 × 10−6 rad . θR = 1.22λ/D = 6.10 × 10−5 rad =⇒θ/θR ≃0.05218 . Physical check The radius for a one-percent loss is much smaller than the radius of the first dark ring; different image-quality measures probe different parts of the pattern.

Question 6

The Bessel expansion gives the curvature of the central Airy peak

For a circular aperture, I/Ic=[2J1(u)/u]2I/I_c=[2J_1(u)/u]^2 with u=πDsin⁡θ/λu=\pi D\sin\theta/\lambda. Use J1(u)=u/2−u3/16+u5/384+O(u7)J_1(u)=u/2-u^3/16+u^5/384+O(u^7). Let D=10.0mmD=10.0\,\mathrm{mm} and λ=500nm\lambda=500\,\mathrm{nm}.

Diagram shown in the original SVG worksheet.

  1. Derive the central intensity expansion through fourth order.

  2. Use its quadratic term to estimate the angle causing a one-percent drop from the peak, and compare with the Rayleigh angle.

Question 6 - Solution

The Bessel expansion gives the curvature of the central Airy peak

Diagram shown in the original SVG worksheet.

(a) Method and calculation

2J1(u)/u=1−u2/8+u4/192+O(u6).2J_1(u)/u=1-u^2/8+u^4/192+O(u^6).I/Ic=1−u2/4+5u4/192+O(u6).\boxed{I/I_c=1-u^2/4+5u^4/192+O(u^6)}.

(b) Interpretation and further calculation

u2/4=0.01⇒u=0.20⇒θ≃0.20λ/(πD)=3.18310×10−6rad.u^2/4=0.01\Longrightarrow u=0.20\Longrightarrow\boxed{\theta\simeq0.20\lambda/(\pi D)=3.18310\times10^{-6}\,\mathrm{rad}}.θR=1.22λ/D=6.10×10−5rad⇒θ/θR≃0.05218.\theta_R=1.22\lambda/D=6.10\times10^{-5}\,\mathrm{rad}\Longrightarrow\boxed{\theta/\theta_R\simeq0.05218}.

Physical check

The radius for a one-percent loss is much smaller than the radius of the first dark ring; different image-quality measures probe different parts of the pattern.