Fiber Optics
ECE 422L
2013
• Consultation Time: 2:30 – 4:30 PM
• Main Book:
• Fiber Optics Communications Technology
– by Djafar K. Mynbaev
• OPTICAL FIBER COMMUNICATION
– SUDHEESH
2
VMG
UM Core Values
Excellence
Honesty and Integrity
Teamwork
Innovation
History
• Willebrord Snell
– a Dutch mathematician who in 1621 wrote the formula
for the principle of refraction
• Daniel Colladon and Jaques Babinet
– First demonstrated in the 1840s, The light-guiding
principle behind optical fibers
• John Tyndall (Irish inventor)
– offering public displays using water-fountains .
5
History
• Alexander Graham Bell
– In 1880, demonstrated his photophone, one of the first
true attempts to carry complex signals with light. It was
also the first device to transmit signals wirelessly.
• William Wheeler
– in 1880, the same year that Bell’s photophone made its
debut, used pipes with a reflective coating inside that
guided light from a central arc light throughout a house.
6
History
• Brian O’Brien,
– President of the Optical Society of America
– In 1951 suggested to use a surrounding, or
“cladding,” the fiber with a layer of material
with a lower refractive index.
• Narinder Kapany coined the term fiber
optics
7
History
• In 1966 Charles K. Kao and George
Hockham proposed optical fibers at STC
Laboratories (STL), Harlow, when they
showed that the losses of 1000 db/km in
existing glass (compared to 5-10 db/km in
coaxial cable) was due to contaminants,
which could potentially be removed.
8
History
• AT&T and GTE
– The first full-scale commercial application of
fiber optic communication systems occurred in
1977
– Use fiber optic telephone systems for
commercial customers.
9
Fiber Optics
• Is a glass or plastic fiber designed to guide light
along its length by confining as much light as
possible in a propagating form.
• Are widely used in fiber-optic communication,
which permits transmission over longer distances
and at higher data rates than other forms of wired
and wireless communications.
10
Principles of Fiber Optic Transmission
• The Fiber Optic Link
components
– Transmitter
– Receiver
– The optical fiber
– The connectors
11
• Transmitter
– converts an electrical signal into light energy to
be carried through the fiber optic link.
– The signal could be generated by a computer, a
voice over a telephone, or data from an
industrial sensor.
12
The Fiber Optic link
• Receiver
– Is an electronic device that collects light energy
and converts it into electrical energy, which can
then be converted into its original form.
– The receiver typically consists of a photo
detector to convert the received light into
electricity, and circuitry to amplify and process
the signal.
13
The Fiber Optic link
• Optical Fibers
– Carry light energy from the transmitter to the
receiver. An optical fiber may be made of glass
or plastic, depending on the requirements of the
job that it will perform.
– The advantage: can carry light around corners
and over great distances.
14
The Fiber Optic link
• Connectors
– Attached to the optical fiber
and allows it to be mated to
the transmitter or receiver to
provide solid contact.
– Must align the fiber end
precisely with the light
source or receiver to prevent
signal loss.
15
The Fiber Optic link
Basic Principles of Light
• All light is a form of electromagnetic
energy.
• Electromagnetic energy is emitted by any
object that has a temperature above absolute
zero , which means that the atoms in the
object are in motion.
16
• The energy takes two forms:
– an electrical field and a magnetic field, formed
at right angles to each other and at right angles
to their path of travel,
17
Basic Principles of Light
18
• Light travels at lower velocities through
various materials or media such as the
earth’s atmosphere, glass, plastic, and
water.
• A medium’s optical density, which is
different from its physical density,
determines how quickly light passes
through it.
19
Basic Principles of Light
Refraction
• the bending of light as it
passes from one material
into another.
• occurs when light waves
change speed as they cross
the boundary between two
materials with different
optical densities.
20
• Light slows down
at a denser medium
21
Refraction
22
Refraction Index
Refraction of Light
23
Model used to calculate Refraction
24
• Snell’s law
• n1sinθ1 = n2sinθ2
Critical Angle
• The incident angle required to produce
a refracted angle of 90°.
• As the incident ray moves from normal
toward the critical angle, less and less
of the incident ray’s energy is carried
into the refracted ray.
25
Critical Angle
• Incidence angle < Critical angle
n1
n2
𝜃1
𝜃2
26
Critical Angle
• Incidence angle =
Critical angle
• At the critical angle,
all of the incident
ray’s energy is
refracted along the
interface.
n1
n2
𝜃1
𝜃2 = 90 𝑜
27
Critical Angle
• Incidence angle >
Critical angle
• As the incident
angle exceeds
90°, the light is
reflected
n1
n2
𝜃1 𝜃2
28
Solving for Critical Angle
 θc = arcsin (n2 ÷ n1)
• So if we want to know the critical angle of
an optical fiber having a core RI of n1 = 1.51
and a cladding RI of n2 = 1.46:
 θc = arcsin(1.46 ÷ 1.51) = 75.211°
29
Total Internal Reflection
• Occurs when
Incidence angle >
critical angle
• All light reflects back
toward the incident
medium
30
31
Total Internal Reflection
31
Sample Problem
• Calculate the critical angle of an optical
fiber with a core RI of 1.48 and a
cladding RI of 1.46.
32
Fresnel Reflections
• Reflected at an angle equal to the angle of
incidence.
• The greater the difference in RI between the
two materials, the more light will be
reflected.
• You experience Fresnel reflection whenever
you look through a window and see a faint
reflection of yourself in the glass.
33
• Augustin Fresnel determined how to
calculate the amount of light lost through
Fresnel reflection
• equation: ρ = ((n1 – n2) ÷ (n1 + n2))2
– where ρ is the amount of light reflected and n is
the RI of the medium.
• To calculate the loss in decibels
– dB = 10Log10 (1 – ρ)
34
Fresnel Reflections
Sample
• Calculate the dB loss due to Fresnel
reflection of a light from the air entering
a fiber core with an RI of 1.48.
35
Reference
• Fiber Optics Communications Technology
– by Djafar K. Mynbaev
• OPTICAL FIBER COMMUNICATION
– SUDHEESH
36
37

Fiber optics101

  • 1.
  • 2.
    • Consultation Time:2:30 – 4:30 PM • Main Book: • Fiber Optics Communications Technology – by Djafar K. Mynbaev • OPTICAL FIBER COMMUNICATION – SUDHEESH 2
  • 3.
  • 4.
    UM Core Values Excellence Honestyand Integrity Teamwork Innovation
  • 5.
    History • Willebrord Snell –a Dutch mathematician who in 1621 wrote the formula for the principle of refraction • Daniel Colladon and Jaques Babinet – First demonstrated in the 1840s, The light-guiding principle behind optical fibers • John Tyndall (Irish inventor) – offering public displays using water-fountains . 5
  • 6.
    History • Alexander GrahamBell – In 1880, demonstrated his photophone, one of the first true attempts to carry complex signals with light. It was also the first device to transmit signals wirelessly. • William Wheeler – in 1880, the same year that Bell’s photophone made its debut, used pipes with a reflective coating inside that guided light from a central arc light throughout a house. 6
  • 7.
    History • Brian O’Brien, –President of the Optical Society of America – In 1951 suggested to use a surrounding, or “cladding,” the fiber with a layer of material with a lower refractive index. • Narinder Kapany coined the term fiber optics 7
  • 8.
    History • In 1966Charles K. Kao and George Hockham proposed optical fibers at STC Laboratories (STL), Harlow, when they showed that the losses of 1000 db/km in existing glass (compared to 5-10 db/km in coaxial cable) was due to contaminants, which could potentially be removed. 8
  • 9.
    History • AT&T andGTE – The first full-scale commercial application of fiber optic communication systems occurred in 1977 – Use fiber optic telephone systems for commercial customers. 9
  • 10.
    Fiber Optics • Isa glass or plastic fiber designed to guide light along its length by confining as much light as possible in a propagating form. • Are widely used in fiber-optic communication, which permits transmission over longer distances and at higher data rates than other forms of wired and wireless communications. 10
  • 11.
    Principles of FiberOptic Transmission • The Fiber Optic Link components – Transmitter – Receiver – The optical fiber – The connectors 11
  • 12.
    • Transmitter – convertsan electrical signal into light energy to be carried through the fiber optic link. – The signal could be generated by a computer, a voice over a telephone, or data from an industrial sensor. 12 The Fiber Optic link
  • 13.
    • Receiver – Isan electronic device that collects light energy and converts it into electrical energy, which can then be converted into its original form. – The receiver typically consists of a photo detector to convert the received light into electricity, and circuitry to amplify and process the signal. 13 The Fiber Optic link
  • 14.
    • Optical Fibers –Carry light energy from the transmitter to the receiver. An optical fiber may be made of glass or plastic, depending on the requirements of the job that it will perform. – The advantage: can carry light around corners and over great distances. 14 The Fiber Optic link
  • 15.
    • Connectors – Attachedto the optical fiber and allows it to be mated to the transmitter or receiver to provide solid contact. – Must align the fiber end precisely with the light source or receiver to prevent signal loss. 15 The Fiber Optic link
  • 16.
    Basic Principles ofLight • All light is a form of electromagnetic energy. • Electromagnetic energy is emitted by any object that has a temperature above absolute zero , which means that the atoms in the object are in motion. 16
  • 17.
    • The energytakes two forms: – an electrical field and a magnetic field, formed at right angles to each other and at right angles to their path of travel, 17 Basic Principles of Light
  • 18.
  • 19.
    • Light travelsat lower velocities through various materials or media such as the earth’s atmosphere, glass, plastic, and water. • A medium’s optical density, which is different from its physical density, determines how quickly light passes through it. 19 Basic Principles of Light
  • 20.
    Refraction • the bendingof light as it passes from one material into another. • occurs when light waves change speed as they cross the boundary between two materials with different optical densities. 20
  • 21.
    • Light slowsdown at a denser medium 21 Refraction
  • 22.
  • 23.
  • 24.
    Model used tocalculate Refraction 24 • Snell’s law • n1sinθ1 = n2sinθ2
  • 25.
    Critical Angle • Theincident angle required to produce a refracted angle of 90°. • As the incident ray moves from normal toward the critical angle, less and less of the incident ray’s energy is carried into the refracted ray. 25
  • 26.
    Critical Angle • Incidenceangle < Critical angle n1 n2 𝜃1 𝜃2 26
  • 27.
    Critical Angle • Incidenceangle = Critical angle • At the critical angle, all of the incident ray’s energy is refracted along the interface. n1 n2 𝜃1 𝜃2 = 90 𝑜 27
  • 28.
    Critical Angle • Incidenceangle > Critical angle • As the incident angle exceeds 90°, the light is reflected n1 n2 𝜃1 𝜃2 28
  • 29.
    Solving for CriticalAngle  θc = arcsin (n2 ÷ n1) • So if we want to know the critical angle of an optical fiber having a core RI of n1 = 1.51 and a cladding RI of n2 = 1.46:  θc = arcsin(1.46 ÷ 1.51) = 75.211° 29
  • 30.
    Total Internal Reflection •Occurs when Incidence angle > critical angle • All light reflects back toward the incident medium 30
  • 31.
  • 32.
    Sample Problem • Calculatethe critical angle of an optical fiber with a core RI of 1.48 and a cladding RI of 1.46. 32
  • 33.
    Fresnel Reflections • Reflectedat an angle equal to the angle of incidence. • The greater the difference in RI between the two materials, the more light will be reflected. • You experience Fresnel reflection whenever you look through a window and see a faint reflection of yourself in the glass. 33
  • 34.
    • Augustin Fresneldetermined how to calculate the amount of light lost through Fresnel reflection • equation: ρ = ((n1 – n2) ÷ (n1 + n2))2 – where ρ is the amount of light reflected and n is the RI of the medium. • To calculate the loss in decibels – dB = 10Log10 (1 – ρ) 34 Fresnel Reflections
  • 35.
    Sample • Calculate thedB loss due to Fresnel reflection of a light from the air entering a fiber core with an RI of 1.48. 35
  • 36.
    Reference • Fiber OpticsCommunications Technology – by Djafar K. Mynbaev • OPTICAL FIBER COMMUNICATION – SUDHEESH 36
  • 37.