Young's Interference Experiment — Question 9

Section 35-3 · Physics pages 5768–5769

Question 9 Counting bright orders requires respecting the propagating-angle limit Two ideal pointlike coherent apertures separated by d = 2.20 µm radiate at wavelength λ = 500 nm. For normal illumination, bright orders satisfy d sin θ = mλ. Count only forward directions with −90◦< θ < 90◦. Ignore any aperture envelope. d Schematic; labels, not drawing lengths, specify the data. (a) Determine all allowed integer orders and the number of bright directions. (b) Find the largest positive bright angle and explain why the next order is absent.
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Question 9 - Solution Counting bright orders requires respecting the propagating-angle limit d (a) Method and calculation | sin θ| < 1 =⇒|m| < d/λ = 4.40. m = −4, −3, . . . , 3, 4; N = 9 . (b) Interpretation and further calculation θ4 = sin−1(4/4.4) = 65.380◦. m = 5 : sin θ5 = 5/4.4 > 1 =⇒no propagating order . Physical check This is a geometrical existence limit, distinct from a bright order being suppressed by a finite-slit diffraction envelope.

Question 9

Counting bright orders requires respecting the propagating-angle limit

Two ideal pointlike coherent apertures separated by d=2.20μmd=2.20\,\mu\mathrm m radiate at wavelength λ=500nm\lambda=500\,\mathrm{nm}. For normal illumination, bright orders satisfy dsin⁡θ=mλd\sin\theta=m\lambda. Count only forward directions with −90∘<θ<90∘-90^\circ<\theta<90^\circ. Ignore any aperture envelope.

Diagram shown in the original SVG worksheet.

  1. Determine all allowed integer orders and the number of bright directions.

  2. Find the largest positive bright angle and explain why the next order is absent.

Question 9 - Solution

Counting bright orders requires respecting the propagating-angle limit

Diagram shown in the original SVG worksheet.

(a) Method and calculation

|sin⁡θ|<1⇒|m|<d/λ=4.40.|\sin\theta|<1\Longrightarrow|m|<d/\lambda=4.40.m=−4,−3,…,3,4;N=9.\boxed{m=-4,-3,\ldots,3,4;\quad N=9}.

(b) Interpretation and further calculation

θ4=sin⁡−1(4/4.4)=65.380∘.\boxed{\theta_4=\sin^{-1}(4/4.4)=65.380^\circ}.m=5:sin⁡θ5=5/4.4>1⇒no propagating order.m=5:\quad\sin\theta_5=5/4.4>1\Longrightarrow\boxed{\text{no propagating order}}.

Physical check

This is a geometrical existence limit, distinct from a bright order being suppressed by a finite-slit diffraction envelope.