Polarization — Question 6

Section 33-6 · Physics pages 5482–5483

Question 6 A diagonal analyzer detects coherence missed by horizontal and vertical tests A monochromatic vacuum beam has Ex = a cos ωt and Ey = b cos(ωt + δ), with positive amplitudes a and b. An ideal analyzer transmits the projection along angle theta from x. x y axis Schematic; labels, not drawing lengths, specify the data. (a) Derive the transmitted cycle-averaged intensity. (b) For a=b, find the 45-degree analyzer intensity for delta=0, pi/2, and pi in units of the total incident intensity.
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Question 6 - Solution A diagonal analyzer detects coherence missed by horizontal and vertical tests x y axis (a) Method and calculation Eθ = a cos θ cos ωt + b sin θ cos(ωt + δ). Iθ = 1 2ϵ0c[a2 cos2 θ + b2 sin2 θ + 2ab cos δ sin θ cos θ] . (b) Interpretation and further calculation a = b : Iin = ϵ0ca2, I45/Iin = (1 + cos δ)/2. I45/Iin = 1, 1/2, 0 for δ = 0, π/2, π . Physical check Horizontal and vertical analyzer readings are independent of delta; the diagonal cross term reveals relative-phase information.

Question 6

A diagonal analyzer detects coherence missed by horizontal and vertical tests

A monochromatic vacuum beam has Ex=acos⁡ωtE_x=a\cos\omega t and Ey=bcos⁡(ωt+δ)E_y=b\cos(\omega t+\delta), with positive amplitudes a and b. An ideal analyzer transmits the projection along angle theta from x.

Diagram shown in the original SVG worksheet.

  1. Derive the transmitted cycle-averaged intensity.

  2. For a=b, find the 45-degree analyzer intensity for delta=0, pi/2, and pi in units of the total incident intensity.

Question 6 - Solution

A diagonal analyzer detects coherence missed by horizontal and vertical tests

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Eθ=acos⁡θcos⁡ωt+bsin⁡θcos⁡(ωt+δ).E_\theta=a\cos\theta\cos\omega t+b\sin\theta\cos(\omega t+\delta).Iθ=12ϵ0c[a2cos⁡2θ+b2sin⁡2θ+2abcos⁡δsin⁡θcos⁡θ].\boxed{I_\theta=\tfrac12\epsilon_0c[a^2\cos^2\theta+b^2\sin^2\theta+2ab\cos\delta\sin\theta\cos\theta]}.

(b) Interpretation and further calculation

a=b:Iin=ϵ0ca2,I45/Iin=(1+cos⁡δ)/2.a=b:\ I_{\mathrm{in}}=\epsilon_0ca^2,\quad I_{45}/I_{\mathrm{in}}=(1+\cos\delta)/2.I45/Iin=1,1/2,0forδ=0,π/2,π.\boxed{I_{45}/I_{\mathrm{in}}=1,\ 1/2,\ 0\quad\text{for}\quad\delta=0,\pi/2,\pi}.

Physical check

Horizontal and vertical analyzer readings are independent of delta; the diagonal cross term reveals relative-phase information.