Intensity in Single-Slit Diffraction, Qualitatively — Question 4

Section 36-3 · Physics pages 5898–5899

Question 4 Adjacent diffraction lobes can have opposite field signs For a centered uniformly illuminated slit, choose the far-field amplitude F(β) = Fc sin β/β real, with positive Fc. Compare β = π/2 and β = 3π/2. A weak coherent reference can reveal the field sign. β/π F Schematic; labels, not drawing lengths, specify the data. (a) Find the signed field at both points and their relative phase. (b) Find the ratio of their intensities and explain what an intensity-only image misses.
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Question 4 - Solution Adjacent diffraction lobes can have opposite field signs β/π F (a) Method and calculation F(π/2) = 2Fc/π, F(3π/2) = −2Fc/(3π) . ∆arg F = π (mod 2π) . (b) Interpretation and further calculation I(3π/2)/I(π/2) = 1/9 . |F|2 = | −F|2 =⇒intensity alone does not retain the field sign . Physical check Crossing a simple amplitude zero reverses the field sign even though the recorded intensity remains nonnegative.

Question 4

Adjacent diffraction lobes can have opposite field signs

For a centered uniformly illuminated slit, choose the far-field amplitude F(β)=Fcsin⁡β/βF(\beta)=F_c\sin\beta/\beta real, with positive FcF_c. Compare β=π/2\beta=\pi/2 and β=3π/2\beta=3\pi/2. A weak coherent reference can reveal the field sign.

Diagram shown in the original SVG worksheet.

  1. Find the signed field at both points and their relative phase.

  2. Find the ratio of their intensities and explain what an intensity-only image misses.

Question 4 - Solution

Adjacent diffraction lobes can have opposite field signs

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F(π/2)=2Fc/π,F(3π/2)=−2Fc/(3π).\boxed{F(\pi/2)=2F_c/\pi,\quad F(3\pi/2)=-2F_c/(3\pi)}.Δarg⁡F=π(mod⁡2π).\boxed{\Delta\arg F=\pi\pmod{2\pi}}.

(b) Interpretation and further calculation

I(3π/2)/I(π/2)=1/9.\boxed{I(3\pi/2)/I(\pi/2)=1/9}.|F|2=|−F|2⇒intensity alone does not retain the field sign.|F|^2=|-F|^2\Longrightarrow\boxed{\text{intensity alone does not retain the field sign}}.

Physical check

Crossing a simple amplitude zero reverses the field sign even though the recorded intensity remains nonnegative.