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Fiber Optic Transmission SL/HL – Option F Mr. Jean

Fiber Optic Transmission SL/HL – Option F Mr. Jean

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Page 1: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Fiber Optic Transmission

SL/HL – Option F

Mr. Jean

Page 2: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Reflection/Refraction

• Reflection– A wave encounters a boundary between two

mediums and cannot pass through– The angle of incidence is always equal to the

angle of reflection

• Refraction– When a wave passes through boundary into a

new medium its speed changes– The wave will change directions based on the

change in its speed

Page 3: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Refraction

• If the wave speeds up it will bend away from the normal line

• If the wave slows down it will bend towards the normal line

• Snell’s Lawsin sini i r rn n

Page 4: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Critical Angle

• When traveling into air from some medium, light will always speed up, thus increasing the angle– If it speeds up enough, the angle of refraction will

be 90 degrees• This means that the refracted ray will travel along the

edge of the boundary

Page 5: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Critical Angle

• When light strikes the boundary at the critical angle or greater, the wave is totally reflected back into the first medium

• Here n1 is the index of refraction of the medium the light starts in

Page 6: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Total Internal Reflection

• Usually when a wave reaches a boundary between mediums it is partially reflected and partially refracted– When the critical angle is

exceeded the entire wave is reflected back within the medium

– The wave doesn’t lose any energy

Page 7: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Optical Fiber

• Fiber optic cable is made of thin, clear glass or plastic

• Once light enters the cable it is totally internally reflected until it reaches the far end– Actual optical fiber is step indexed• There is another layer between

the core and the outside• This is so the fibers can be

bundled together

Page 8: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Fibre Optics:

• https://www.youtube.com/watch?v=0MwMkBET_5I

• https://www.youtube.com/watch?v=12OSBJwogFc

Page 9: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Dispersion

• Modal– Not all the waves that enter make it to the other

end, only certain ones– The possible paths are called modes

• Material– Because different frequencies have different

refractive indices, they have different paths• These can both cause problems if the bits of

data arrive out of order • More direct modes are faster• Laser light and single mode cable reduce

these effects

Page 10: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Material Dispersion

Page 11: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Attenuation

• Attenuation is the opposite of amplification– As a signal travels through a cable it will slowly

lose intensity as energy is lost– Attenuation is measured in decibels (dB)

• The 10 at the beginning is to convert to decibels• Generally measured in dBkm-1

10 10

10 log ( ) 10log ( )

i

o

PPower inattenuation

Power out P

Page 12: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Attenuation

• Attenuation is the opposite of amplification– As a signal travels through a cable it will slowly

lose intensity as energy is lost– Attenuation is measured in decibels (dB)

• The 10 at the beginning is to convert to decibels• Generally measured in dBkm-1

10 10

10 log ( ) 10log ( )

i

o

PPower inattenuation

Power out P

Page 13: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 14: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 15: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 16: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Wavelength & Attenuation

Page 17: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 18: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Noise

• One advantage to using fiber optics is that it is not particularly susceptible to noise– Any noise that does occur is generally due to

random light entering the end of the cable– The power ratio of noise to signal in fiber optics is

generally in the range of 10-17 or 10-18

Page 19: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Re-shapers

• Mono-mode fibers can eliminate modal dispersion and lasers cut down on material dispersion, but it is not completely eliminated– Over a long distance individual pulses can start to

overlap each other– Every 40-60km is a reshaper which will detect and

reshape the signal• Has its own laser which sends a ‘new’ signal

Page 20: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Amplifiers

• Even with reshaping, signals still attenuate over the length of the cable– Amplifiers along the cable increase the signal

strength to keep it going

– https://phet.colorado.edu/en/simulation/lasers

Page 21: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 22: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 23: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Textbook Questions: P. 638-639

Page 24: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 25: Fiber Optic Transmission SL/HL – Option F Mr. Jean

Textbook Questions:

Page 26: Fiber Optic Transmission SL/HL – Option F Mr. Jean
Page 27: Fiber Optic Transmission SL/HL – Option F Mr. Jean