Diffraction — Question 4

Section 35-2 · Physics pages 5738–5739

Question 4 Paired Huygens sources explain the first dark direction Divide a uniformly illuminated slit of width a into two equal halves. Pair each point u in the lower half with the point u + a/2 in the upper half. In the far field at angle θ, the pair path difference is (a/2) sin θ. Assume equal amplitudes and scalar waves. a/2 parallel far-field rays Schematic; labels, not drawing lengths, specify the data. (a) Derive the smallest positive angle at which every such pair cancels. (b) For a = 0.80 µm and λ = 0.60 µm, find that angle and decide whether the same construction has a physical first-zero angle if a is reduced to 0.40 µm.
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Question 4 - Solution Paired Huygens sources explain the first dark direction a/2 parallel far-field rays (a) Method and calculation ∆ϕpair = 2π λ a 2 sin θ = π. a sin θ1 = λ ; E(u) + E(u + a/2) = 0. (b) Interpretation and further calculation θ1 = sin−1(0.60/0.80) = 48.590◦. a = 0.40 µm : sin θ1 = 1.50 > 1 ⇒no propagating first-zero direction in this model . Physical check The absence of a first zero does not mean the absence of diffraction; the angular distribution becomes very broad.

Question 4

Paired Huygens sources explain the first dark direction

Divide a uniformly illuminated slit of width a into two equal halves. Pair each point u in the lower half with the point u+a/2u+a/2 in the upper half. In the far field at angle θ\theta, the pair path difference is (a/2)sin⁡θ(a/2)\sin\theta. Assume equal amplitudes and scalar waves.

Diagram shown in the original SVG worksheet.

  1. Derive the smallest positive angle at which every such pair cancels.

  2. For a=0.80μma=0.80\,\mu\mathrm m and λ=0.60μm\lambda=0.60\,\mu\mathrm m, find that angle and decide whether the same construction has a physical first-zero angle if a is reduced to 0.40μm0.40\,\mu\mathrm m.

Question 4 - Solution

Paired Huygens sources explain the first dark direction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Δϕpair=2πλa2sin⁡θ=π.\Delta\phi_{\mathrm{pair}}=\frac{2\pi}{\lambda}\frac a2\sin\theta=\pi.asin⁡θ1=λ;E(u)+E(u+a/2)=0.\boxed{a\sin\theta_1=\lambda};\quad E(u)+E(u+a/2)=0.

(b) Interpretation and further calculation

θ1=sin⁡−1(0.60/0.80)=48.590∘.\boxed{\theta_1=\sin^{-1}(0.60/0.80)=48.590^\circ}.a=0.40μm:sin⁡θ1=1.50>1⇒no propagating first-zero direction in this model.a=0.40\,\mu\mathrm m:\quad\sin\theta_1=1.50>1\Rightarrow\boxed{\text{no propagating first-zero direction in this model}}.

Physical check

The absence of a first zero does not mean the absence of diffraction; the angular distribution becomes very broad.