Diffraction — Question 7

Section 35-2 · Physics pages 5744–5745

Question 7 An aperture integral reveals why rescaling the opening rescales the pattern The far-field amplitude of a uniformly illuminated slit is proportional to Aa(q) = ∫a/2 −a/2 eiqu du, where q = k sin θ. Define the normalized amplitude Fa(q) = Aa(q)/Aa(0). Consider a new slit of width sa, with positive scale factor s. a sa θ Schematic; labels, not drawing lengths, specify the data. (a) Use a change of integration variable to derive the scaling law for the normalized amplitude. (b) For s = 3, determine the new angle corresponding to a fixed feature originally at θ = 6.0◦ and give its small-angle limit.
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Question 7 - Solution An aperture integral reveals why rescaling the opening rescales the pattern a sa θ (a) Method and calculation Asa(q) = ∫sa/2 −sa/2 eiqudu = s ∫a/2 −a/2 ei(sq)vdv = sAa(sq). Asa(0) = sAa(0) =⇒Fsa(q) = Fa(sq) . (b) Interpretation and further calculation sk sin θ′ = k sin θ =⇒θ′ = sin−1(sin 6◦/3) = 1.99675◦. |θ| ≪1 : θ′ ≃θ/s = 2.0◦. Physical check Normalization removes the increase in on-axis amplitude; only the angular contraction remains in this comparison.

Question 7

An aperture integral reveals why rescaling the opening rescales the pattern

The far-field amplitude of a uniformly illuminated slit is proportional to Aa(q)=∫−a/2a/2eiquduA_a(q)=\int_{-a/2}^{a/2}e^{iqu}\,du, where q=ksin⁡θq=k\sin\theta. Define the normalized amplitude Fa(q)=Aa(q)/Aa(0)F_a(q)=A_a(q)/A_a(0). Consider a new slit of width sasa, with positive scale factor s.

Diagram shown in the original SVG worksheet.

  1. Use a change of integration variable to derive the scaling law for the normalized amplitude.

  2. For s=3s=3, determine the new angle corresponding to a fixed feature originally at θ=6.0∘\theta=6.0^\circ and give its small-angle limit.

Question 7 - Solution

An aperture integral reveals why rescaling the opening rescales the pattern

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Asa(q)=∫−sa/2sa/2eiqudu=s∫−a/2a/2ei(sq)vdv=sAa(sq).A_{sa}(q)=\int_{-sa/2}^{sa/2}e^{iqu}du=s\int_{-a/2}^{a/2}e^{i(sq)v}dv=sA_a(sq).Asa(0)=sAa(0)⇒Fsa(q)=Fa(sq).A_{sa}(0)=sA_a(0)\Longrightarrow\boxed{F_{sa}(q)=F_a(sq)}.

(b) Interpretation and further calculation

sksin⁡θ′=ksin⁡θ⇒θ′=sin⁡−1(sin⁡6∘/3)=1.99675∘.sk\sin\theta^\prime=k\sin\theta\Longrightarrow\boxed{\theta^\prime=\sin^{-1}(\sin6^\circ/3)=1.99675^\circ}.|θ|≪1:θ′≃θ/s=2.0∘.|\theta|\ll1:\quad\boxed{\theta^\prime\simeq\theta/s=2.0^\circ}.

Physical check

Normalization removes the increase in on-axis amplitude; only the angular contraction remains in this comparison.