Intensity in Double-Slit Interference — Question 1

Section 35-5 · Physics pages 5792–5793

Question 1 Adding field phasors gives the intensity at an arbitrary phase Two coherent, parallel-polarized waves in the same medium have peak electric-field amplitudes E0 and 2E0. Define I0 as the intensity of the first wave alone. Their relative phase is δ = 120◦. E0 2E0 eE Schematic; labels, not drawing lengths, specify the data. (a) Add the field phasors and obtain the intensity at this phase. (b) Find the maximum and minimum possible intensities and their visibility as the phase is varied.
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Question 1 - Solution Adding field phasors gives the intensity at an arbitrary phase E0 2E0 eE (a) Method and calculation eE = E0(1 + 2eiδ), I/I0 = |1 + 2eiδ|2 = 5 + 4 cos δ. I(120◦) = 3I0 . (b) Interpretation and further calculation Imax = (1 + 2)2I0 = 9I0, Imin = (2 −1)2I0 = I0 . V = 9 −1 9 + 1 = 0.80 . Physical check Field amplitudes add before squaring. A phase difference of pi cannot fully cancel beams with unequal amplitudes.

Question 1

Adding field phasors gives the intensity at an arbitrary phase

Two coherent, parallel-polarized waves in the same medium have peak electric-field amplitudes E0E_0 and 2E02E_0. Define I0I_0 as the intensity of the first wave alone. Their relative phase is δ=120∘\delta=120^\circ.

Diagram shown in the original SVG worksheet.

  1. Add the field phasors and obtain the intensity at this phase.

  2. Find the maximum and minimum possible intensities and their visibility as the phase is varied.

Question 1 - Solution

Adding field phasors gives the intensity at an arbitrary phase

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Ẽ=E0(1+2eiδ),I/I0=|1+2eiδ|2=5+4cos⁡δ.\widetilde E=E_0(1+2e^{i\delta}),\quad I/I_0=|1+2e^{i\delta}|^2=5+4\cos\delta.I(120∘)=3I0.\boxed{I(120^\circ)=3I_0}.

(b) Interpretation and further calculation

Imax=(1+2)2I0=9I0,Imin=(2−1)2I0=I0.\boxed{I_{\max}=(1+2)^2I_0=9I_0,\quad I_{\min}=(2-1)^2I_0=I_0}.V=9−19+1=0.80.\boxed{V=\frac{9-1}{9+1}=0.80}.

Physical check

Field amplitudes add before squaring. A phase difference of pi cannot fully cancel beams with unequal amplitudes.