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Fibre Optics


         by

Dr. Amit Kumar Chawla
Optical Fibre

Optical Fibre is an optical transmission device which
works on the principle of total internal reflection.

          Principle of Optical Fibre
When a light signal is directed at one end of the fibre at
a suitable angle, it undergoes repeated total internal
reflection along the length of the fibre and finally
comes out at the other end.
Optical Fiber
• Core
   – Glass or plastic with a higher index of
     refraction than the cladding
   – Carries the signal
• Cladding
   – Glass or plastic with a lower index of
     refraction than the core
• Buffer
   – Protects the fiber from damage and
     moisture
• Jacket
   – Holds one or more fibers in a cable
Potential low cost: The glass which generally provides
the optical fiber transmission medium is made from
sand (SiO2).
Enormous band width: The optical carrier frequency in
the range 1013 to 1016 Hz.
In metallic cable systems band width is 500-700 MHz's.
The amount of data that can be transmitted in a fixed
amount of time.
Signal security: Optical fibers provides the high degree
of signal security.

Using an Optical fiber, 15000 independent speeches
can be sent where as using a pair of copper wires,
only 48 independent speeches can be sent
Types of Optical Fibre (Based on core size)




Single Mode Step             Multimode Fibre
Index Fibre




                   Multimode           Multimode
                   Step Index Fibres   Graded Index Fibres
Single Mode Step Index Fiber
• Single mode step index fiber has a core diameter
of 8 to 9 microns, which only allows one light path
or mode
• Single mode fibres have a lower signal loss and
  a higher information capacity or bandwidth than
  a multimode fibre.




                                           Index of
                                           refraction
Multimode Step-Index Fiber
• Multimode fiber has a core diameter of 50 to 100
  microns (sometimes even larger)
  – Allows several light paths (~100) or modes
   – This causes modal dispersion – some modes
     take longer to pass through the fiber than others
     because they travel a longer distance




                                                  Index of
                                                  refraction
Multimode Graded-Index Fiber
• The index of refraction gradually changes
  across the core
  – Modes that travel further also move faster
  – This reduces modal dispersion so the bandwidth is
    greatly increased




                                                  Index of
                                                  refraction
Step-index and Graded-index
• Step index multimode was developed first,
  but rare today because it has a low
  bandwidth (50 MHz-km)
• It has been replaced by graded-index
  multimode with a bandwidth up to 2 GHz-
  km
Fiber Optic Specifications
• Attenuation
  – Loss of signal, measured in dB
• Dispersion
  – Blurring of a signal, affects bandwidth
• Bandwidth
  – The number of bits per second that can be
    sent through a data link
• Numerical Aperture
  – Measures the largest angle of light that can
    be accepted into the core
Acceptance Angle
Optical fibre will only propagate light that enters the fibre within
a certain cone, known as acceptance cone of the fibre. The
half-angle of this cone is called the acceptance angle (θi)

                                 Cladding ( µ 2 )
 Air ( µo )               θ                    Core( µ1 )
                 φ
        i                                            Axis



   From Snell’s law
                         µo sin i = µ1 sin φ
φ = 90 − θ
                                o


               µo sin i = µ1 sin(90o − θ )

              µo sin i = µ1 cos θ
          µo sin i = µ1 1 − sin θ   2



If i increases, Φ increases and θ decreases.

There is a maximum value of i beyond which the light ray
entering the fibre will fall on the core-cladding interface at
an angle less than θc. Such a ray will be refracted into the
cladding and will not propagate. This maximum value of i,
say imax is called the acceptance angle of the fibre.
µo sin imax = µ1 1 − sin θ c
                                      2




When   θ = θ c then according to Snell’s law
                    µ1 sin 90o
                       =
                    µ 2 sin θ c
                              µ2
                    sin θ c =
                              µ1

            µo sin imax = µ1 1 − ( µ 2 µ1 )
                                              2




               µo sin imax = µ12 − µ 2
                                     2
Taking µ o   =1   for air, we get


                   sin imax = µ − µ 2
                                    1
                                        2
                                        2

This equation gives a relation between the acceptance
angle and the refractive indices of the core and the
cladding.

The cone associated with the angle imax is called the
acceptance cone.
Numerical Aperture
It is the measure of the light gathering capacity of the fibre
and is defined as the product of sine of the acceptance
angle and the refractive index of the medium to which the
end faces of the fibre are exposed.

                     NA = µo sin imax
Taking µ o   =1   for air, we get

              NA = sin imax = µ − µ  2
                                     1
                                          2
                                          2



                          µ1 − µ 2
Relative index       ∆µ =
                             µ1
The General Communication
         System
The Optical fibre Communication
             System
ATTENUATION
  Attenuation or transmission loss is the loss of optical power
  as light travels down a fiber.

  The decrease in signal strength along a fiber optic
  waveguide caused by absorption and scattering is known as
  attenuation.

  Attenuation is usually expressed in dB/km

Since attenuation is the loss, therefore, it is always expressed as

                                                    Pin
                                      αL = 10 log10
                                                    Pout
    where α is the attenuation coefficient of the fiber
Dispersion
Dispersion, expressed in terms of the symbol ∆t, is
defined as pulse spreading in an optical fibre. As a pulse
of light propagates through a fibre, elements such as
numerical aperture, core diameter, refractive index
profile, wavelength, and laser line width cause the pulse
to broaden. This poses a limitation on the overall
bandwidth of the fibre.
V Number
 The number of modes of multimode fiber cable depends on
 the wavelength of light, core diameter and material
 composition. This can be determined by the Normalized
 frequency parameter (V).
                 πd            πd
              V=    µ1 − µ 2 =
                     2     2
                                  NA
                  λ             λ
 Where , d = fiber core diameter ;    λ = wavelength of light
 NA=numerical aperture

For a single mode fiber, V ≤ 2.4 and for multimode fiber, V ≥
2.4.
Mathematically, the number of modes for a fiber is given by:



       For Step-index                   For Graded-index

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physics b.tech. 1st sem fibre optics,u 4

  • 1. Fibre Optics by Dr. Amit Kumar Chawla
  • 2. Optical Fibre Optical Fibre is an optical transmission device which works on the principle of total internal reflection. Principle of Optical Fibre When a light signal is directed at one end of the fibre at a suitable angle, it undergoes repeated total internal reflection along the length of the fibre and finally comes out at the other end.
  • 3. Optical Fiber • Core – Glass or plastic with a higher index of refraction than the cladding – Carries the signal • Cladding – Glass or plastic with a lower index of refraction than the core • Buffer – Protects the fiber from damage and moisture • Jacket – Holds one or more fibers in a cable
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  • 6. Potential low cost: The glass which generally provides the optical fiber transmission medium is made from sand (SiO2). Enormous band width: The optical carrier frequency in the range 1013 to 1016 Hz. In metallic cable systems band width is 500-700 MHz's. The amount of data that can be transmitted in a fixed amount of time. Signal security: Optical fibers provides the high degree of signal security. Using an Optical fiber, 15000 independent speeches can be sent where as using a pair of copper wires, only 48 independent speeches can be sent
  • 7. Types of Optical Fibre (Based on core size) Single Mode Step Multimode Fibre Index Fibre Multimode Multimode Step Index Fibres Graded Index Fibres
  • 8. Single Mode Step Index Fiber • Single mode step index fiber has a core diameter of 8 to 9 microns, which only allows one light path or mode • Single mode fibres have a lower signal loss and a higher information capacity or bandwidth than a multimode fibre. Index of refraction
  • 9. Multimode Step-Index Fiber • Multimode fiber has a core diameter of 50 to 100 microns (sometimes even larger) – Allows several light paths (~100) or modes – This causes modal dispersion – some modes take longer to pass through the fiber than others because they travel a longer distance Index of refraction
  • 10. Multimode Graded-Index Fiber • The index of refraction gradually changes across the core – Modes that travel further also move faster – This reduces modal dispersion so the bandwidth is greatly increased Index of refraction
  • 11. Step-index and Graded-index • Step index multimode was developed first, but rare today because it has a low bandwidth (50 MHz-km) • It has been replaced by graded-index multimode with a bandwidth up to 2 GHz- km
  • 12. Fiber Optic Specifications • Attenuation – Loss of signal, measured in dB • Dispersion – Blurring of a signal, affects bandwidth • Bandwidth – The number of bits per second that can be sent through a data link • Numerical Aperture – Measures the largest angle of light that can be accepted into the core
  • 13. Acceptance Angle Optical fibre will only propagate light that enters the fibre within a certain cone, known as acceptance cone of the fibre. The half-angle of this cone is called the acceptance angle (θi) Cladding ( µ 2 ) Air ( µo ) θ Core( µ1 ) φ i Axis From Snell’s law µo sin i = µ1 sin φ
  • 14. φ = 90 − θ o µo sin i = µ1 sin(90o − θ ) µo sin i = µ1 cos θ µo sin i = µ1 1 − sin θ 2 If i increases, Φ increases and θ decreases. There is a maximum value of i beyond which the light ray entering the fibre will fall on the core-cladding interface at an angle less than θc. Such a ray will be refracted into the cladding and will not propagate. This maximum value of i, say imax is called the acceptance angle of the fibre.
  • 15. µo sin imax = µ1 1 − sin θ c 2 When θ = θ c then according to Snell’s law µ1 sin 90o = µ 2 sin θ c µ2 sin θ c = µ1 µo sin imax = µ1 1 − ( µ 2 µ1 ) 2 µo sin imax = µ12 − µ 2 2
  • 16. Taking µ o =1 for air, we get sin imax = µ − µ 2 1 2 2 This equation gives a relation between the acceptance angle and the refractive indices of the core and the cladding. The cone associated with the angle imax is called the acceptance cone.
  • 17. Numerical Aperture It is the measure of the light gathering capacity of the fibre and is defined as the product of sine of the acceptance angle and the refractive index of the medium to which the end faces of the fibre are exposed. NA = µo sin imax Taking µ o =1 for air, we get NA = sin imax = µ − µ 2 1 2 2 µ1 − µ 2 Relative index ∆µ = µ1
  • 19. The Optical fibre Communication System
  • 20. ATTENUATION Attenuation or transmission loss is the loss of optical power as light travels down a fiber. The decrease in signal strength along a fiber optic waveguide caused by absorption and scattering is known as attenuation. Attenuation is usually expressed in dB/km Since attenuation is the loss, therefore, it is always expressed as Pin αL = 10 log10 Pout where α is the attenuation coefficient of the fiber
  • 21. Dispersion Dispersion, expressed in terms of the symbol ∆t, is defined as pulse spreading in an optical fibre. As a pulse of light propagates through a fibre, elements such as numerical aperture, core diameter, refractive index profile, wavelength, and laser line width cause the pulse to broaden. This poses a limitation on the overall bandwidth of the fibre.
  • 22. V Number The number of modes of multimode fiber cable depends on the wavelength of light, core diameter and material composition. This can be determined by the Normalized frequency parameter (V). πd πd V= µ1 − µ 2 = 2 2 NA λ λ Where , d = fiber core diameter ; λ = wavelength of light NA=numerical aperture For a single mode fiber, V ≤ 2.4 and for multimode fiber, V ≥ 2.4. Mathematically, the number of modes for a fiber is given by: For Step-index For Graded-index