The ray is reflected along the water and air boundary. At this point θ1 is known as the critical angle θc
The ray is reflected back at the water boundary. This partial reflection where θ3 = θ1
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Total Internal Reflection 2
The law of refraction states that n1sinθ1 =n2sinθ2
When the refracted ray passes directly across the boundary the incident ray is striking the boundary at the critical angle θc
n1sinθ1 = n2sinθ2
Since sin90 = 1, n1sinθc = n2
Sinθc = n2/n1
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Refraction in Optical Fibres
The light is refracted as it enters the fibre. Since the refractive index of air is 1: Sinθ = (1/n2) sinθ where n2 is the refractive index of the glass (usually about 1.5)
In effect, θ1 > θ2 so the ray refracts towards the normal
The ray proceeds inside the fibre until it is incident upon the boundary. Provided that the angle of incidence at this event (θ3 = 90 - θ2) is greater than the critical angle, total internal reflection will occur and the ray will be trapped inside the fibre,
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Structure of Optical Fibres
The simplest kind of optical fibre is a thin piece of glass or other transparent medium
An effective improvement on the simple fibre is to wrap the core fibre in a material known as cladding. The cladding protects the core from scratches or moisture that may enable light to leak out. This allows information to be transmitted with a greater degree of security.
Multimodal dispersion occurs in simple optical fibres with a low critical angle (about 42) as there are many paths that the ray can follow. For example in an extreme case, yellow reaches the reciever before the red ray (which has travelled further)
To reduce multimodal dispersion you can use monochromatic light and increase the critical angle by making the core thinner and the cladding thicker
Coherent Signals-What is coming in is the same as what is coming out.
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