The Light-Emitting Diode (LED) — Question 5

Section 41-9 · Physics pages 6960–6961

Question 5 Total internal reflection restricts a planar escape cone Photons are emitted isotropically inside a semiconductor of refractive index n = 2.50 adjoining air through one planar face. Ignore Fresnel reflection, absorption, and repeated encounters. Only rays within the critical-angle cone toward that face escape on the first encounter. air n θc Schematic; labels, not drawing lengths, specify the data. (a) Find the critical angle and the escaping fraction of all emission directions. (b) Use the large-n approximation to estimate that fraction and compare with the exact value.
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Question 5 - Solution Total internal reflection restricts a planar escape cone air n θc (a) Method and calculation θc = sin−1(1/n) = 23.58◦. fesc = 2π ∫θc 0 sin θ dθ 4π = 1 −cos θc 2 = .04174 . (b) Interpretation and further calculation cos θc = √ 1 −1/n2 ≃1 −1/(2n2). fesc ≃1/(4n2) = .0400 (4.17% below exact). Physical check The denominator includes all directions, not only the upward hemisphere. This is a first-pass geometric fraction; coatings, texturing and photon recycling alter extraction.

Question 5

Total internal reflection restricts a planar escape cone

Photons are emitted isotropically inside a semiconductor of refractive index n=2.50n=2.50 adjoining air through one planar face. Ignore Fresnel reflection, absorption, and repeated encounters. Only rays within the critical-angle cone toward that face escape on the first encounter.

Diagram shown in the original SVG worksheet.

  1. Find the critical angle and the escaping fraction of all emission directions.

  2. Use the large-n approximation to estimate that fraction and compare with the exact value.

Question 5 - Solution

Total internal reflection restricts a planar escape cone

Diagram shown in the original SVG worksheet.

(a) Method and calculation

θc=sin⁡−1(1/n)=23.58∘.\boxed{\theta_c=\sin^{-1}(1/n)=23.58^\circ}.fesc=2π∫0θcsin⁡θdθ4π=1−cos⁡θc2=.04174.\boxed{f_{\mathrm{esc}}=\frac{2\pi\int_0^{\theta_c}\sin\theta\,d\theta}{4\pi}=\frac{1-\cos\theta_c}{2}=.04174}.

(b) Interpretation and further calculation

cos⁡θc=1−1/n2≃1−1/(2n2).\cos\theta_c=\sqrt{1-1/n^2}\simeq1-1/(2n^2).fesc≃1/(4n2)=.0400(4.17% below exact).\boxed{f_{\mathrm{esc}}\simeq1/(4n^2)=.0400}\quad(4.17\%\text{ below exact}).

Physical check

The denominator includes all directions, not only the upward hemisphere. This is a first-pass geometric fraction; coatings, texturing and photon recycling alter extraction.