Diffraction by a Double Slit — Question 10

Section 36-6 · Physics pages 5970–5971

Question 10 Opposite illumination tilts can separate the two diffraction envelopes Two equal slits have normalized field factors f1(β) = sinc(β −b) and f2(β) = sinc(β + b) because their incident wavefront tilts differ. Set b = π/2. A controllable relative phase is scanned; V = 2|f1f2|/(|f1|2 + |f2|2) where the denominator is nonzero. d P slit width a Schematic; labels, not drawing lengths, specify the data. (a) Calculate visibility at β = 0 and the maximum normalized intensity there. (b) Calculate visibility and normalized intensity at β = π/2. Use unit intensity for a single field factor of magnitude one.
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Question 10 - Solution Opposite illumination tilts can separate the two diffraction envelopes d P slit width a (a) Method and calculation β = 0 : f1 = f2 = 2/π =⇒V = 1 . Imax(0) = (4/π)2 = 16/π2 . (b) Interpretation and further calculation β = π/2 : f1 = 1, f2 = 0 =⇒V = 0 . I(π/2) = 1 independent of relative phase . Physical check Equal slit widths do not guarantee equal amplitudes at every observation angle when the incident phase slopes differ.

Question 10

Opposite illumination tilts can separate the two diffraction envelopes

Two equal slits have normalized field factors f1(β)=sinc⁡(β−b)f_1(\beta)=\operatorname{sinc}(\beta-b) and f2(β)=sinc⁡(β+b)f_2(\beta)=\operatorname{sinc}(\beta+b) because their incident wavefront tilts differ. Set b=π/2b=\pi/2. A controllable relative phase is scanned; V=2|f1f2|/(|f1|2+|f2|2)V=2|f_1f_2|/(|f_1|^2+|f_2|^2) where the denominator is nonzero.

Diagram shown in the original SVG worksheet.

  1. Calculate visibility at β=0\beta=0 and the maximum normalized intensity there.

  2. Calculate visibility and normalized intensity at β=π/2\beta=\pi/2. Use unit intensity for a single field factor of magnitude one.

Question 10 - Solution

Opposite illumination tilts can separate the two diffraction envelopes

Diagram shown in the original SVG worksheet.

(a) Method and calculation

β=0:f1=f2=2/π⇒V=1.\beta=0:\quad f_1=f_2=2/\pi\Longrightarrow\boxed{V=1}.Imax(0)=(4/π)2=16/π2.\boxed{I_{\max}(0)=(4/\pi)^2=16/\pi^2}.

(b) Interpretation and further calculation

β=π/2:f1=1,f2=0⇒V=0.\beta=\pi/2:\quad f_1=1,\ f_2=0\Longrightarrow\boxed{V=0}.I(π/2)=1independent of relative phase.\boxed{I(\pi/2)=1\quad\text{independent of relative phase}}.

Physical check

Equal slit widths do not guarantee equal amplitudes at every observation angle when the incident phase slopes differ.