Intensity in Double-Slit Interference — Question 10

Section 35-5 · Physics pages 5810–5811

Question 10 Intensity near a dark fringe gives a quadratic displacement signal Two equal coherent beams form a dark fringe at y = yd. Near it, write I(y) = 4I0 sin2[π(y −yd)/p], where p is fringe spacing and 4I0 is the bright level. Let p = 2.0 mm. y I yd Schematic; labels, not drawing lengths, specify the data. (a) Derive the leading quadratic intensity and find the displacement magnitude that produces one percent of the bright level using the exact expression. (b) Compare with the quadratic estimate and explain the sign ambiguity of the inferred displacement.
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Question 10 - Solution Intensity near a dark fringe gives a quadratic displacement signal y I yd (a) Method and calculation sin x ≃x =⇒I ≃4I0π2(y −yd)2/p2 . I/(4I0) = 0.01 =⇒|y −yd| = p π sin−1(0.1) = 63.7686 µm . (b) Interpretation and further calculation |y −yd|quad = 0.1p/π = 63.6620 µm . I(yd + η) = I(yd −η) =⇒η = ±63.7686 µm locally . Physical check The quadratic estimate is slightly smaller than the exact displacement. A dark-fringe intensity cannot determine which side of the minimum the detector occupies.

Question 10

Intensity near a dark fringe gives a quadratic displacement signal

Two equal coherent beams form a dark fringe at y=ydy=y_d. Near it, write I(y)=4I0sin⁡2[π(y−yd)/p]I(y)=4I_0\sin^2[\pi(y-y_d)/p], where p is fringe spacing and 4I04I_0 is the bright level. Let p=2.0mmp=2.0\,\mathrm{mm}.

Diagram shown in the original SVG worksheet.

  1. Derive the leading quadratic intensity and find the displacement magnitude that produces one percent of the bright level using the exact expression.

  2. Compare with the quadratic estimate and explain the sign ambiguity of the inferred displacement.

Question 10 - Solution

Intensity near a dark fringe gives a quadratic displacement signal

Diagram shown in the original SVG worksheet.

(a) Method and calculation

sin⁡x≃x⇒I≃4I0π2(y−yd)2/p2.\sin x\simeq x\Longrightarrow\boxed{I\simeq4I_0\pi^2(y-y_d)^2/p^2}.I/(4I0)=0.01⇒|y−yd|=pπsin⁡−1(0.1)=63.7686μm.I/(4I_0)=0.01\Longrightarrow\boxed{|y-y_d|=\frac p\pi\sin^{-1}(0.1)=63.7686\,\mu\mathrm m}.

(b) Interpretation and further calculation

|y−yd|quad=0.1p/π=63.6620μm.\boxed{|y-y_d|_{\mathrm{quad}}=0.1p/\pi=63.6620\,\mu\mathrm m}.I(yd+η)=I(yd−η)⇒η=±63.7686μmlocally.I(y_d+\eta)=I(y_d-\eta)\Longrightarrow\boxed{\eta=\pm63.7686\,\mu\mathrm m\ \text{locally}}.

Physical check

The quadratic estimate is slightly smaller than the exact displacement. A dark-fringe intensity cannot determine which side of the minimum the detector occupies.