Diffraction by a Double Slit — Question 5

Section 36-6 · Physics pages 5960–5961

Question 5 Unequal slit widths produce angle-dependent visibility Two uniformly illuminated slits have widths a and 2a, with the same incident field amplitude A0. At fixed q their individual amplitudes are F1 = A0a sinc β and F2 = 2A0a sinc(2β), where β = qa/2. A controlled phase is scanned between them. d P widths a, 2a Schematic; labels, not drawing lengths, specify the data. (a) Find the on-axis visibility. (b) At β = π/2, find the visibility and intensity relative to the in-phase on-axis intensity of both slits.
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Question 5 - Solution Unequal slit widths produce angle-dependent visibility d P widths a, 2a (a) Method and calculation q = 0 : |F1| : |F2| = 1 : 2 =⇒V0 = 2(1)(2) 12 + 22 = 0.80 . Ic,both ∝|A0a + 2A0a|2 = 9A2 0a2. (b) Interpretation and further calculation β = π/2 : F1 = 2A0a/π, F2 = 0 =⇒V = 0 . I/Ic,both = 4/(9π2) = 0.0450316 . Physical check At the wider slit’s first zero, only the narrower slit contributes, so changing relative phase cannot modulate the intensity.

Question 5

Unequal slit widths produce angle-dependent visibility

Two uniformly illuminated slits have widths a and 2a, with the same incident field amplitude A0A_0. At fixed q their individual amplitudes are F1=A0asinc⁡βF_1=A_0a\operatorname{sinc}\beta and F2=2A0asinc⁡(2β)F_2=2A_0a\operatorname{sinc}(2\beta), where β=qa/2\beta=qa/2. A controlled phase is scanned between them.

Diagram shown in the original SVG worksheet.

  1. Find the on-axis visibility.

  2. At β=π/2\beta=\pi/2, find the visibility and intensity relative to the in-phase on-axis intensity of both slits.

Question 5 - Solution

Unequal slit widths produce angle-dependent visibility

Diagram shown in the original SVG worksheet.

(a) Method and calculation

q=0:|F1|:|F2|=1:2⇒V0=2(1)(2)12+22=0.80.q=0:\quad |F_1|:|F_2|=1:2\Longrightarrow\boxed{V_0=\frac{2(1)(2)}{1^2+2^2}=0.80}.Ic,both∝|A0a+2A0a|2=9A02a2.I_{c,\mathrm{both}}\propto|A_0a+2A_0a|^2=9A_0^2a^2.

(b) Interpretation and further calculation

β=π/2:F1=2A0a/π,F2=0⇒V=0.\beta=\pi/2:\quad F_1=2A_0a/\pi,\quad F_2=0\Longrightarrow\boxed{V=0}.I/Ic,both=4/(9π2)=0.0450316.\boxed{I/I_{c,\mathrm{both}}=4/(9\pi^2)=0.0450316}.

Physical check

At the wider slit’s first zero, only the narrower slit contributes, so changing relative phase cannot modulate the intensity.