Diffraction by a Double Slit — Question 6

Section 36-6 · Physics pages 5962–5963

Question 6 A half-cycle phase offset changes the number of central-envelope bright orders Equal slits have d/a = 2.50. A uniform phase plate adds relative phase pi, so the intensity is I = 4Is sinc2 β sin2 α, with α = πd sin θ/λ and β = (a/d)α. d P slit width a π plate Schematic; labels, not drawing lengths, specify the data. (a) Find the nominal bright-order condition and classify the axis. (b) Count the nominal bright directions strictly inside the central envelope and determine whether the envelope-edge orders survive.
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Question 6 - Solution A half-cycle phase offset changes the number of central-envelope bright orders d P slit width a π plate (a) Method and calculation sin2 α = 1 =⇒α = (m + 1/2)π ; α = 0 =⇒I = 0 . |β| < π =⇒|m + 1/2| < 2.50. (b) Interpretation and further calculation m + 1/2 = −1.5, −0.5, 0.5, 1.5 : 4 directions . m + 1/2 = ±2.5 =⇒β = ±π =⇒both edge orders are missing . Physical check A phase plate shifts the interference factor but leaves the individual slit envelope fixed.

Question 6

A half-cycle phase offset changes the number of central-envelope bright orders

Equal slits have d/a=2.50d/a=2.50. A uniform phase plate adds relative phase pi, so the intensity is I=4Issinc⁡2βsin⁡2αI=4I_s\operatorname{sinc}^2\beta\sin^2\alpha, with α=πdsin⁡θ/λ\alpha=\pi d\sin\theta/\lambda and β=(a/d)α\beta=(a/d)\alpha.

Diagram shown in the original SVG worksheet.

  1. Find the nominal bright-order condition and classify the axis.

  2. Count the nominal bright directions strictly inside the central envelope and determine whether the envelope-edge orders survive.

Question 6 - Solution

A half-cycle phase offset changes the number of central-envelope bright orders

Diagram shown in the original SVG worksheet.

(a) Method and calculation

sin⁡2α=1⇒α=(m+1/2)π;α=0⇒I=0.\sin^2\alpha=1\Longrightarrow\boxed{\alpha=(m+1/2)\pi};\quad\alpha=0\Longrightarrow\boxed{I=0}.|β|<π⇒|m+1/2|<2.50.|\beta|<\pi\Longrightarrow|m+1/2|<2.50.

(b) Interpretation and further calculation

m+1/2=−1.5,−0.5,0.5,1.5:4directions.\boxed{m+1/2=-1.5,-0.5,0.5,1.5:\ 4\ \text{directions}}.m+1/2=±2.5⇒β=±π⇒both edge orders are missing.m+1/2=\pm2.5\Longrightarrow\beta=\pm\pi\Longrightarrow\boxed{\text{both edge orders are missing}}.

Physical check

A phase plate shifts the interference factor but leaves the individual slit envelope fixed.