Total Internal Reflection
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Total Internal Reflection
A critical concept in the case of optical fibers is the case total internal reflection. The bending of light as it goes into medium is related to the index of reflection of the materials (n1 and n2). By Snell's law when n1 > n2 then θ 1 is less than θ2. As you decrease the angle θ1 and bring the light closer to parallel with the interface you reach a critical angle θ1c where there is total internal reflection.
Snells laws are also known as Fresnel's Equations:
- <math>\theta _i = \theta _r\,\!</math>
and
- <math>\frac {sin \theta_i} {\theta_t} = \frac {n_2} {n_1}\,\!</math>
where
- <math>\theta_i\,\!</math> is the angle of incidence
- <math>\theta_r\,\!</math> is the angle of reflection
- <math>\theta_{c} = sin^{-1}(\frac {n_2} {n_1} )\,\!</math>
where:
- <math>\theta_{c}\,\!</math> is the critical angle
- <math>n_1 , n_2\,\!</math> are the index of refraction of the two media
if θ1 keeps Increasing: θ2 approaches 90°
for a critical angle Θ1, Θ2 = 90°and the beam emerges along the surface
When θ2 = 90° → sin θ2 = 1
If θi > θc then there is total reflection and there is no transmitted light in the second medium (the irradiance of the reflected and incident beams is equal). Light interacts at the interface and there is a phase shift between the incident and the reflected beams which is dependent on the two materials.
tan psi
This is a critical process in optical fibers and waveguides because it can carry light for long distances. For these values of index of refraction you get a critical angle of 78.6 which means the light must be very nearly parallel to the interface.
for n1 = 1.53 and n2 = 1.50 : θ1c = 78.6°
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