Diffraction and the Wave Theory of Light — Question 5

Section 36-1 · Physics pages 5860–5861

Question 5 Fresnel similarity requires distance to scale with aperture size squared For one-dimensional paraxial propagation use U(x, L) = C(L) ∫a/2 −a/2 A(u) exp[iπ(x −u)2/(λL)]du. Compare geometrically similar normalized aperture profiles after scaling all transverse coordinates by s, at fixed wavelength. a P L a →sa, L →s2L Schematic; labels, not drawing lengths, specify the data. (a) Find how L must scale to leave the phase kernel unchanged. (b) If the slit width grows from 0.20 to 0.60 mm, find the new propagation distance and feature coordinate corresponding to L = 0.40 m and x = 0.80 mm.
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Question 5 - Solution Fresnel similarity requires distance to scale with aperture size squared a P L a →sa, L →s2L (a) Method and calculation u′ = su, x′ = sx : (x′ −u′)2 λL′ = s2(x −u)2 λL′ . L′ = s2L =⇒same normalized Fresnel pattern. (b) Interpretation and further calculation s = 0.60/0.20 = 3 =⇒L′ = 3.60 m . x′ = sx = 2.40 mm . Physical check This is a near-field similarity transformation. Scaling distance linearly with aperture width would not preserve the quadratic phase.

Question 5

Fresnel similarity requires distance to scale with aperture size squared

For one-dimensional paraxial propagation use U(x,L)=C(L)∫−a/2a/2A(u)exp⁡[iπ(x−u)2/(λL)]duU(x,L)=C(L)\int_{-a/2}^{a/2}A(u)\exp[i\pi(x-u)^2/(\lambda L)]du. Compare geometrically similar normalized aperture profiles after scaling all transverse coordinates by s, at fixed wavelength.

Diagram shown in the original SVG worksheet.

  1. Find how L must scale to leave the phase kernel unchanged.

  2. If the slit width grows from 0.200.20 to 0.60mm0.60\,\mathrm{mm}, find the new propagation distance and feature coordinate corresponding to L=0.40mL=0.40\,\mathrm m and x=0.80mmx=0.80\,\mathrm{mm}.

Question 5 - Solution

Fresnel similarity requires distance to scale with aperture size squared

Diagram shown in the original SVG worksheet.

(a) Method and calculation

u′=su,x′=sx:(x′−u′)2λL′=s2(x−u)2λL′.u^\prime=su,\quad x^\prime=sx:\quad\frac{(x^\prime-u^\prime)^2}{\lambda L^\prime}=\frac{s^2(x-u)^2}{\lambda L^\prime}.L′=s2L⇒same normalized Fresnel pattern.\boxed{L^\prime=s^2L}\Longrightarrow\text{same normalized Fresnel pattern}.

(b) Interpretation and further calculation

s=0.60/0.20=3⇒L′=3.60m.s=0.60/0.20=3\Longrightarrow\boxed{L^\prime=3.60\,\mathrm m}.x′=sx=2.40mm.\boxed{x^\prime=sx=2.40\,\mathrm{mm}}.

Physical check

This is a near-field similarity transformation. Scaling distance linearly with aperture width would not preserve the quadratic phase.