OPTICAL FIBRE IN COMMUNICATION

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Presentation transcript:

OPTICAL FIBRE IN COMMUNICATION Shubha Gokhale School of Sciences, IGNOU

Optical Fibres in Communication 2

Advantages of OF Communication High information capacity of fibre: digital communication bit-rates of up to 14 Tbit s-1 have been reached over a single 160 km line Low attenuation and dispersion: <0.3 dB km1 Space saving: due to extreme thin dimensions (total diameter < 500 μm) of fibre the coefficient of information capacity to cable cross section is high Low cross-talk: does not generate any interference to other systems 3

Advantages of OF Communication (Contd…) Immunity to EMI: free from EMI pick ups, including lightening, sparking etc. Higher security: no radiation of EM waves involved hence tapping difficult Low cost: relative to the metallic coaxial cables and due to wide spacing between the repeaters. Abundance of basic resource: Silica Easy maintainability 4

Limitations of OF Systems Optical fibre needs special technique of splicing to connect to other fibre. Due to small dimensions the fibre coupling needs great accuracy in alignment (of few m) Every time the signal needs amplification, it needs to be first converted to electrical signal, then amplified using electronic amplifiers and then again converted back into optical signal 5

Working Principle of OF 6

Critical Angle Snell’s Law n1 sin 1 = n2 sin 2 where 1 is angle of incidence and 2 is angle of refraction At critical angle, C , 2 = 90 sin 2=1 7

Construction of Optical Fibre Core refractive index (n1) > cladding refractive index (n2) Typical diameter of core ~ 5-10 μm Cladding diameter ~10-15 times core diameter 8

Acceptance Angle a is the maximum angle to the axis at which light may get propagated in the fibre and is called the acceptance angle. 9

n0 sin θa is known as Numerical Aperture n0 sin 1 = n1 sin 2 = n1 cos  for 1 = a = C n0 sin θa is known as Numerical Aperture 10

Example A silica optical fibre with a core diameter of 30 m has core refractive index of 1.50 and a cladding refractive index of 1.47. Its input end is immersed in water. Calculate : the critical angle at the core-cladding interface the NA for the fibre the acceptance angle for the fibre in water (Refractive index of water is 1.33) 11

Critical Angle Determination The critical angle c at the core-cladding interface is given by 12

Numerical Aperture Calculation The numerical aperture is given by: 13

Acceptance Angle in Water Acceptance angle in water can be obtained by using : 14

Modes of Optical Transmission Geometric optics approach does not hold good for small diameters The ray theory model describes only the direction of a plane wave component in the fibre It does not take into account interference between such components. Due to interference phenomena only rays with certain discrete characteristics propagate in the fibre core. Fibre supports only limited number of discrete guided modes. 15

Modes in Optical Fibres A mode is a stable propagation state in an optical fibre. The number of modes that can be propagated in a fibre depends on  Refractive index of core and cladding core diameter wavelength of the propagating light The core diameter can be reduced to achieve single mode of operation. 16

Classification of Optical Fibres Based on the number of modes propagating in a fibre: Single-mode (SM) fibre Multi-mode (MM) fibre Based on the gradient of refractive index value of core : Step index (SI) fibre Graded index (GI) fibre 17

Step Index Fibres SI SM SI MM 18

Graded Index Fibre GI MM 19

Signal Attenuation in Fibre Signal gets attenuated while getting transmitted through the fibre L = 10 log10 (Pout / Pin) Depending upon the attenuation, spacing between the repeaters is decided 20

Intrinsic Losses in Fibre Losses occurring due to fibre material and structure imperfection Rayleigh scattering due to structure imperfection Absorption by (impurity) ions in the fibre Geometric parameter variation Microbending 21

Extrinsic Losses in the Fibre Losses occurring due to external factors Fibre connection losses Splicing losses Connector losses Fibre bending losses 22

Telecommunication Windows Preferred wavelengths of operation: 850 nm 1310 nm 1550 nm 23

Chromatic dispersion Also known as Material Dispersion Caused by variation of refractive index with wavelength of the light passing through the material Different wavelength (colour) light travel with different speeds and emerge out at different times Usually does not affect normal operation as single wavelengths are used in communication 24

GI MM fibre can take care of modal dispersion to some extent Different Modes GI MM fibre can take care of modal dispersion to some extent 25

Modal Dispersion and Data Handling Optical fibre is mostly used for handling digital (binary) signals in form of pulses Number of bits transmitted per second determine the capacity of data handling If modal dispersion widens the pulse, the spacing between two pulses needs to be increased in order to avoid inter-mixing of consecutive pulses. This reduces the capacity Advisable to reduce the modal dispersion 26

Optical Communication System Apart from fibres, optical communication system comprises of opto-electronic converters : Electrical – optical converter has optical source driven by electrical signal Optical – electrical converter has optical detector that senses signal emerging out of fibre and produces corresponding electrical pulses 27

Optical Sources Incandescent light LED Laser Diodes Sources should be small, focused for better fibre coupling Incandescent lights not preferred due to its white nature 28

Optical Sources :LED Light Emitting Diode is a semiconductor diode with direct band gap materials Monochromatic, small size, easy fabrication GaAs: IR AlGaAs: Red GaAsP, GaP: Orange, Yellow InGaN/GaN: Green ZnSe: Blue ZnSe/ Phosphor: White 29

Optical Sources : Laser Diode Laser diodes are degeneratively doped semiconductor p-n junctions made of direct band gap materials Highly monochromatic, coherent, small divergence, high intensity InGaN : Blue-violet AlGaAs: Green AlGaInP: Red, IR 30

Characteristics of Optical Sources 31

Optical Detectors : Photodiode Reverse biased semiconductor junction diode with depletion and diffusion regions. Diffusion is slow process hence detection bandwidth is low. 32

Optical Detector : p-i-n Diode This geometry allows absorption of photon in larger area (intrinsic layer that acts as wider depletion region) 33

Applications of Optical Fibres Communication Sensors Illumination Light guides in medical field Imaging optics in endoscopy Sunlight guide for buildings Decorations Light conduction in spectrometers 34

Thank You! 35