fresnel equations and em power flow
DESCRIPTION
Fresnel Equations and EM Power Flow. Reading - Shen and Kong – Ch. 4. Outline Review of Oblique Incidence Review of Snell ’ s Law Fresnel Equations Evanescence and TIR Brewster ’ s Angle EM Power Flow. TRUE / FALSE. H r. This EM wave is TE (transverse electric) polarized: - PowerPoint PPT PresentationTRANSCRIPT
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Fresnel Equations and EM Power Flow
Outline
• Review of Oblique Incidence• Review of Snell’s Law• Fresnel Equations• Evanescence and TIR• Brewster’s Angle • EM Power Flow
Reading - Shen and Kong – Ch. 4
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TRUE / FALSE
1. This EM wave is TE(transverse electric) polarized:
2. Snell’s Law only works for TE polarized light.
3. Total internal reflection only occurs when light goes from a high index material to a low index material.
Ei
EtEr
Hi
Ht
Hr
•y
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Refraction
Refraction involves a change in the direction of wave propagation due to a change in propagation speed. It involves the oblique incidence of waves on media boundaries, and hence wave propagation in at least two dimensions.
Water Waves E&M Waves
Waves refract at the top where the water is shallower
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flick
r
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Refraction in Suburbia
Think of refraction as a pair of wheels on an axle going from a sidewalk onto grass. The wheel in the grass moves slower, so the direction of the wheel pair changes.
Note that the wheelsmove faster (longer space)on the sidewalk, and slower(shorter space) in the grass.
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Moreover, this wheel analogy is mathematically equivalent to the refraction phenomenon. One can
recover Snell’s law from it: n1sin1 = n2sin2 .
The upper wheel hits the sidewalk and starts to go faster, which turns the axle until the upper wheel re-enters the grass and wheel
pair goes straight again.
Total Internal Reflection in Suburbia
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Oblique Incidence (3D view)
Boundary
y
xki
z
kiz kix
θi
kix = ki sin(θi)
kiz = ki cos(θi)
Identical definitions for kr and kt
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Oblique Incidence at Dielectric Interface
TransverseElectric Field
TransverseMagnetic Field
Ei
Et
Et
Ei
Er
Er
Hi
Hi
Ht
Ht
Hr
Hr
•y Why do we consider only these two polarizations?
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Partial TE Analysis
Ei
EtEr
Hi
Ht
Hr
•y
Tangential E must be continuous at the boundary z = 0 for all x and for t.
z = 0
This is possible if and only if kix = krx = ktx and ωi = ωr = ωt. The former condition is phase matching.
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Snell’s Law Diagram
Tangential E field is continuous …
Refraction Total Internal Reflection
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Snell’s Law
•
Snell’s Law
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TE Analysis - Set Up
Ei
EtEr
Hi
Ht
Hr
•y
z = 0
θi θt
θr
ki
krkt
Medium 1 Medium 2
To get H, use Faraday’s Law
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TE Analysis – Boundary Conditions
Incident Wavenumber:
Phase Matching:
Tangential E:
Normal μH:
Tangential H:
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Solution Boundary conditions are:
Ei
EtEr
Hi
Ht
Hr
•y
z = 0
θi θt
θr
ki
krkt
Medium 1 Medium 2
Fresnel Equations
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Today’s Culture MomentSir David Brewster
1781 –1868
• Scottish scientist• Studied at University of Edinburgh at age 12• Independently discovered Fresnel lens• Editor of Edinburgh Encyclopedia and contributor to Encyclopedia Britannica (7th and 8th editions)• Inventor of the Kaleidoscope• Nominated (1849) to the National Institute of France.
Kaleidoscope
Fresnel Lens
All Images are in the public domain
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TM Case is the dual of TE
E Gauss: k∙E = 0
H Gauss: k∙H = 0
Faraday: k х E = ωμH
Ampere: k х H = - ωεE
E Gauss: k∙E = 0
H Gauss: k∙H = 0
Faraday: k х E = ωμH
Ampere: k х H = - ωεE
E → H
H → - E
ε → μ
μ → ε
The TM solution can be recovered from the TE solution. So, consider only the TE solution in detail.
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TE & TM Analysis – Solution
TE solution comes directly from the boundary condition analysis
TM solution comes from ε ↔ μ
Note that the TM solution provides the reflection and transmission coefficients for H, since TM is the dual of TE.
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Fresnel Equations - Summary
TM Polarization
TE-polarization
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Fresnel Equations - Summary
TE Polarization TM Polarization
From Shen and Kong … just another way of writing the same results
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Fresnel Equations
Ei
Et
Et
Ei
Er
Er
Hi
Hi
Ht
Ht
Hr
Hr
•y
TE
TM
rTM
rTE
tTE
tTM
n1 = 1.0 n2 = 1.5
θB
Incidence Angle
Refle
ctio
n Co
efficie
nts
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Fresnel Equations
rTM
rTE
θCθB
θC = sin-1(n2 / n1)
Total Internal Reflection
Ei
Et
Et
Ei
Er
Er
Hi
Hi
Ht
Ht
Hr
Hr
•y
TE
TM
n2 = 1.0n1 = 1.5
Incidence Angle
Refle
ctio
n Co
efficie
nts
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Reflection of Light(Optics Viewpoint … μ1 = μ2)
Incidence Angle
Refle
ctio
n Co
efficie
nts
TE:
TM:
Ei
Et
Et
Ei
Er
Er
Hi
Hi
Ht
Ht
Hr
Hr
•y
TE
TM
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Sir David Brewster
Light incident on the surface is absorbed, and then reradiated by oscillating electric dipoles (Lorentz oscillators) at the interface between the two media. The dipoles that produce the transmitted (refracted) light oscillate in the polarization direction of that light. These same oscillating dipoles also generate the reflected light. However, dipoles do not radiate any energy in the direction along which they oscillate. Consequently, if the direction of the refracted light is perpendicular to the direction in which the light is predicted to be specularly reflected, the dipoles will not create any TM-polarized reflected light.
Brewster’s Angle(Optics Viewpoint … μ1 = μ2)
UnpolarizedIncident Ray
TE PolarizedReflected Ray
Slightly PolarizedReflracted Ray
Snell’s LawRequiresn1 = n2
Snell’s LawCan beSatisfied with
θB = arctan(n2/n1)
θB + θT = 90°
Image in the Public Domain
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Cross-sectional Areas
Energy Transport
TE
TM
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Transmitted Power Fraction:
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Reflected Power Fraction:
… and from ENERGY CONSERVATION we know:
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Summary CASE I:
E-field is polarized perpendicular to the plane of incidence
… then E-field is parallel (tangential) to the surface, and continuity of tangential fields requires that:
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Summary CASE II:
H-field is polarized perpendicular to the plane of incidence
… then H-field is parallel (tangential) to the surface, and continuity of tangential fields requires that:
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