Reflection and Refraction — Question 6

Section 33-7 · Physics pages 5502–5503

Question 6 An electric-field transmission coefficient is not a power fraction At normal incidence between lossless nonmagnetic media, the electric amplitude coefficients are r = (n1 −n2)/(n1 + n2) and t = 2n1/(n1 + n2). Intensity for peak electric amplitude E is nϵ0cE2/2. Take n1=1 and n2=1.5. Ei Er Et Schematic; labels, not drawing lengths, specify the data. (a) Derive the reflected and transmitted power fractions, retaining the intensity prefactor. (b) Evaluate both fractions and the field coefficients, and verify conservation of energy.
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Question 6 - Solution An electric-field transmission coefficient is not a power fraction Ei Er Et (a) Method and calculation R = |r|2, T = n2 n1 |t|2 = 4n1n2 (n1 + n2)2 . R + T = (n1 −n2)2 + 4n1n2 (n1 + n2)2 = 1. (b) Interpretation and further calculation r = −0.20, t = 0.80 . R = 0.040, T = 0.960 , t2 = 0.640̸ = T. Physical check The reflected field changes sign for entry into the larger index; the transmitted energy depends on both field amplitude and medium impedance.

Question 6

An electric-field transmission coefficient is not a power fraction

At normal incidence between lossless nonmagnetic media, the electric amplitude coefficients are r=(n1−n2)/(n1+n2)r=(n_1-n_2)/(n_1+n_2) and t=2n1/(n1+n2)t=2n_1/(n_1+n_2). Intensity for peak electric amplitude E is nϵ0cE2/2n\epsilon_0cE^2/2. Take n1=1 and n2=1.5.

Diagram shown in the original SVG worksheet.

  1. Derive the reflected and transmitted power fractions, retaining the intensity prefactor.

  2. Evaluate both fractions and the field coefficients, and verify conservation of energy.

Question 6 - Solution

An electric-field transmission coefficient is not a power fraction

Diagram shown in the original SVG worksheet.

(a) Method and calculation

R=|r|2,T=n2n1|t|2=4n1n2(n1+n2)2.R=|r|^2,\quad T=\frac{n_2}{n_1}|t|^2=\boxed{\frac{4n_1n_2}{(n_1+n_2)^2}}.R+T=(n1−n2)2+4n1n2(n1+n2)2=1.R+T=\frac{(n_1-n_2)^2+4n_1n_2}{(n_1+n_2)^2}=1.

(b) Interpretation and further calculation

r=−0.20,t=0.80.\boxed{r=-0.20,\quad t=0.80}.R=0.040,T=0.960,t2=0.640≠T.\boxed{R=0.040,\quad T=0.960},\quad t^2=0.640\ne T.

Physical check

The reflected field changes sign for entry into the larger index; the transmitted energy depends on both field amplitude and medium impedance.