Diffraction — Question 2

Section 35-2 · Physics pages 5734–5735

Question 2 The quadratic path correction tests a far-field approximation A slit extends from u = −a/2 to u = a/2 and is observed on axis at distance L. The exact path is r(u) = √ L2 + u2. Let a = 1.0 mm, λ = 500 nm. Require the largest neglected quadratic phase to be at most π/10. P L a/2 −a/2 Schematic; labels, not drawing lengths, specify the data. (a) Expand r through second order and express the maximum quadratic phase in terms of a, L, and wavelength. (b) Find the minimum L satisfying the stated phase tolerance.
Show solutionHide solution
Question 2 - Solution The quadratic path correction tests a far-field approximation P L a/2 −a/2 (a) Method and calculation r(u) = L √ 1 + u2/L2 ≃L + u2 2L. ∆ϕmax = 2π λ (a/2)2 2L = πa2 4λL . (b) Interpretation and further calculation πa2 4λL ≤π 10 =⇒L ≥5a2 2λ . Lmin = 5.0 m ; a/Lmin = 2.0 × 10−4. Physical check The small geometrical ratio a/L alone does not guarantee a negligible phase error, because optical wavelengths are very short.

Question 2

The quadratic path correction tests a far-field approximation

A slit extends from u=−a/2u=-a/2 to u=a/2u=a/2 and is observed on axis at distance L. The exact path is r(u)=L2+u2r(u)=\sqrt{L^2+u^2}. Let a=1.0mma=1.0\,\mathrm{mm}, λ=500nm\lambda=500\,\mathrm{nm}. Require the largest neglected quadratic phase to be at most π/10\pi/10.

Diagram shown in the original SVG worksheet.

  1. Expand r through second order and express the maximum quadratic phase in terms of a, L, and wavelength.

  2. Find the minimum L satisfying the stated phase tolerance.

Question 2 - Solution

The quadratic path correction tests a far-field approximation

Diagram shown in the original SVG worksheet.

(a) Method and calculation

r(u)=L1+u2/L2≃L+u22L.r(u)=L\sqrt{1+u^2/L^2}\simeq L+\frac{u^2}{2L}.Δϕmax=2πλ(a/2)22L=πa24λL.\boxed{\Delta\phi_{\max}=\frac{2\pi}{\lambda}\frac{(a/2)^2}{2L}=\frac{\pi a^2}{4\lambda L}}.

(b) Interpretation and further calculation

πa24λL≤π10⇒L≥5a22λ.\frac{\pi a^2}{4\lambda L}\leq\frac{\pi}{10}\Longrightarrow L\geq\frac{5a^2}{2\lambda}.Lmin=5.0m;a/Lmin=2.0×10−4.\boxed{L_{\min}=5.0\,\mathrm m};\qquad a/L_{\min}=2.0\times10^{-4}.

Physical check

The small geometrical ratio a/L alone does not guarantee a negligible phase error, because optical wavelengths are very short.