Diffraction by a Double Slit — Question 1

Section 36-6 · Physics pages 5952–5953

Question 1 Two displaced finite slits multiply an envelope by an interference factor Two equal uniform slits of width a have centers at u = ±d/2. One centered slit has amplitude Fs(q) = A0a sinc(qa/2), with sinc x = sin x/x. Let β = qa/2 and α = qd/2. d P slit width a Schematic; labels, not drawing lengths, specify the data. (a) Use the translation phase factors to derive the total amplitude. (b) Derive the intensity in units of one slit’s axial intensity Is, and identify the two independent zero conditions.
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Question 1 - Solution Two displaced finite slits multiply an envelope by an interference factor d P slit width a (a) Method and calculation F(q) = Fs(q)eiqd/2 + Fs(q)e−iqd/2 = 2A0a sinc β cos α . I = 4Is sinc2 β cos2 α . (b) Interpretation and further calculation β = pπ, p̸ = 0 : envelope zeros . α = (m + 1/2)π : interference zeros . Physical check A dark direction may be caused by either factor; attributing every minimum to slit separation can give an incorrect aperture estimate.

Question 1

Two displaced finite slits multiply an envelope by an interference factor

Two equal uniform slits of width a have centers at u=±d/2u=\pm d/2. One centered slit has amplitude Fs(q)=A0asinc⁡(qa/2)F_s(q)=A_0a\,\operatorname{sinc}(qa/2), with sinc⁡x=sin⁡x/x\operatorname{sinc}x=\sin x/x. Let β=qa/2\beta=qa/2 and α=qd/2\alpha=qd/2.

Diagram shown in the original SVG worksheet.

  1. Use the translation phase factors to derive the total amplitude.

  2. Derive the intensity in units of one slit’s axial intensity IsI_s, and identify the two independent zero conditions.

Question 1 - Solution

Two displaced finite slits multiply an envelope by an interference factor

Diagram shown in the original SVG worksheet.

(a) Method and calculation

F(q)=Fs(q)eiqd/2+Fs(q)e−iqd/2=2A0asinc⁡βcos⁡α.F(q)=F_s(q)e^{iqd/2}+F_s(q)e^{-iqd/2}=\boxed{2A_0a\,\operatorname{sinc}\beta\cos\alpha}.I=4Issinc⁡2βcos⁡2α.\boxed{I=4I_s\operatorname{sinc}^2\beta\cos^2\alpha}.

(b) Interpretation and further calculation

β=pπ,p≠0:envelope zeros.\boxed{\beta=p\pi,\ p\ne0:\ \text{envelope zeros}}.α=(m+1/2)π:interference zeros.\boxed{\alpha=(m+1/2)\pi:\ \text{interference zeros}}.

Physical check

A dark direction may be caused by either factor; attributing every minimum to slit separation can give an incorrect aperture estimate.