Light as a Wave — Question 5

Section 35-1 · Physics pages 5720–5721

Question 5 The sign of a reflection coefficient determines a half-cycle shift At normal incidence the electric-field reflection coefficient from a lossless dielectric is r = (ni −nt)/(ni + nt). Compare reflection A from air (ni = 1) into glass (nt = 1.50) with reflection B from glass into air. Compare phases relative to each local incident field; incident intensities are equal. ni nt rEi Schematic; labels, not drawing lengths, specify the data. (a) Calculate both signed field coefficients and reflection phase changes. (b) Calculate both reflected intensity fractions and the relative reflection phase.
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Question 5 - Solution The sign of a reflection coefficient determines a half-cycle shift ni nt rEi (a) Method and calculation rA = (1 −1.50)/(1 + 1.50) = −0.20 , rB = +0.20 . ϕr,A = π, ϕr,B = 0 (mod 2π) . (b) Interpretation and further calculation RA = |rA|2 = RB = |rB|2 = 0.040 . ϕr,A −ϕr,B = π (mod 2π) . Physical check An intensity measurement loses the sign of the reflected electric field; equal reflectances do not imply equal reflection phases.

Question 5

The sign of a reflection coefficient determines a half-cycle shift

At normal incidence the electric-field reflection coefficient from a lossless dielectric is r=(ni−nt)/(ni+nt)r=(n_i-n_t)/(n_i+n_t). Compare reflection A from air (ni=1n_i=1) into glass (nt=1.50n_t=1.50) with reflection B from glass into air. Compare phases relative to each local incident field; incident intensities are equal.

Diagram shown in the original SVG worksheet.

  1. Calculate both signed field coefficients and reflection phase changes.

  2. Calculate both reflected intensity fractions and the relative reflection phase.

Question 5 - Solution

The sign of a reflection coefficient determines a half-cycle shift

Diagram shown in the original SVG worksheet.

(a) Method and calculation

rA=(1−1.50)/(1+1.50)=−0.20,rB=+0.20.r_A=(1-1.50)/(1+1.50)=\boxed{-0.20},\quad r_B=\boxed{+0.20}.ϕr,A=π,ϕr,B=0(mod⁡2π).\boxed{\phi_{r,A}=\pi,\quad\phi_{r,B}=0\pmod{2\pi}}.

(b) Interpretation and further calculation

RA=|rA|2=RB=|rB|2=0.040.R_A=|r_A|^2=R_B=|r_B|^2=\boxed{0.040}.ϕr,A−ϕr,B=π(mod⁡2π).\boxed{\phi_{r,A}-\phi_{r,B}=\pi\pmod{2\pi}}.

Physical check

An intensity measurement loses the sign of the reflected electric field; equal reflectances do not imply equal reflection phases.