Diffraction and the Wave Theory of Light — Question 3

Section 36-1 · Physics pages 5856–5857

Question 3 Four aperture patches can cancel despite nonzero transmitted power Four equal aperture patches contribute phasors Epeijπ/2 at an observation point, with j = 0, 1, 2, 3. Let Ip be the intensity of one patch alone. The patches are mutually coherent. 1 i −1 −i Schematic; labels, not drawing lengths, specify the data. (a) Find the resultant field and intensity with all four patches open. (b) Find the intensity after patch j = 3 is blocked, and explain why this does not imply increased total transmitted power.
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Question 3 - Solution Four aperture patches can cancel despite nonzero transmitted power 1 i −1 −i (a) Method and calculation E = Ep(1 + i −1 −i) = 0 . I = 0 although each patch transmits nonzero power. (b) Interpretation and further calculation Ethree = Ep(1 + i −1) = iEp =⇒Ithree = Ip . Ptransmitted,three/Ptransmitted,four = 3/4 for equal nonoverlapping patches. Physical check Blocking a patch can brighten one direction by removing cancellation while reducing total transmitted energy.

Question 3

Four aperture patches can cancel despite nonzero transmitted power

Four equal aperture patches contribute phasors Epeijπ/2E_p e^{ij\pi/2} at an observation point, with j=0,1,2,3j=0,1,2,3. Let IpI_p be the intensity of one patch alone. The patches are mutually coherent.

Diagram shown in the original SVG worksheet.

  1. Find the resultant field and intensity with all four patches open.

  2. Find the intensity after patch j=3j=3 is blocked, and explain why this does not imply increased total transmitted power.

Question 3 - Solution

Four aperture patches can cancel despite nonzero transmitted power

Diagram shown in the original SVG worksheet.

(a) Method and calculation

E=Ep(1+i−1−i)=0.E=E_p(1+i-1-i)=\boxed{0}.I=0although each patch transmits nonzero power.\boxed{I=0}\quad\text{although each patch transmits nonzero power}.

(b) Interpretation and further calculation

Ethree=Ep(1+i−1)=iEp⇒Ithree=Ip.E_{\mathrm{three}}=E_p(1+i-1)=iE_p\Longrightarrow\boxed{I_{\mathrm{three}}=I_p}.Ptransmitted,three/Ptransmitted,four=3/4for equal nonoverlapping patches.P_{\mathrm{transmitted,three}}/P_{\mathrm{transmitted,four}}=\boxed{3/4}\quad\text{for equal nonoverlapping patches}.

Physical check

Blocking a patch can brighten one direction by removing cancellation while reducing total transmitted energy.