Polarization — Question 7

Section 33-6 · Physics pages 5484–5485

Question 7 A quarter-wave plate converts equal in-phase components into a circle A lossless plate preserves x and y amplitudes but adds pi/2 to the phase of y relative to x. The incident beam is linearly polarized at 45 degrees, with total electric amplitude E0. input output Schematic; labels, not drawing lengths, specify the data. (a) Write the incident and outgoing component fields and identify the outgoing polarization. (b) Find the transmitted power fraction and the fraction passing a subsequent linear analyzer at any angle.
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Question 7 - Solution A quarter-wave plate converts equal in-phase components into a circle input output (a) Method and calculation Ein = E0 √ 2(ˆx + ˆy) cos ωt. Eout = E0 √ 2(ˆx cos ωt −ˆy sin ωt) , |Eout|2 = E2 0/2. (b) Interpretation and further calculation Iout = Iin = 1 2ϵ0cE2 0 . Iθ = 1 4ϵ0cE2 0(cos2 θ + sin2 θ) ⇒Iθ/Iout = 1/2 . Physical check The field tip moves on a circle. A phase-only plate preserves average power even though instantaneous field magnitude changes.

Question 7

A quarter-wave plate converts equal in-phase components into a circle

A lossless plate preserves x and y amplitudes but adds pi/2 to the phase of y relative to x. The incident beam is linearly polarized at 45 degrees, with total electric amplitude E0.

Diagram shown in the original SVG worksheet.

  1. Write the incident and outgoing component fields and identify the outgoing polarization.

  2. Find the transmitted power fraction and the fraction passing a subsequent linear analyzer at any angle.

Question 7 - Solution

A quarter-wave plate converts equal in-phase components into a circle

Diagram shown in the original SVG worksheet.

(a) Method and calculation

𝑬in=E02(x̂+ŷ)cos⁡ωt.\mathbf E_{\mathrm{in}}=\frac{E_0}{\sqrt2}(\hat x+\hat y)\cos\omega t.𝑬out=E02(x̂cos⁡ωt−ŷsin⁡ωt),|𝑬out|2=E02/2.\boxed{\mathbf E_{\mathrm{out}}=\frac{E_0}{\sqrt2}(\hat x\cos\omega t-\hat y\sin\omega t)},\quad |\mathbf E_{\mathrm{out}}|^2=E_0^2/2.

(b) Interpretation and further calculation

Iout=Iin=12ϵ0cE02.\boxed{I_{\mathrm{out}}=I_{\mathrm{in}}=\tfrac12\epsilon_0cE_0^2}.Iθ=14ϵ0cE02(cos⁡2θ+sin⁡2θ)⇒Iθ/Iout=1/2.I_\theta=\tfrac14\epsilon_0cE_0^2(\cos^2\theta+\sin^2\theta)\Rightarrow\boxed{I_\theta/I_{\mathrm{out}}=1/2}.

Physical check

The field tip moves on a circle. A phase-only plate preserves average power even though instantaneous field magnitude changes.