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Joseph C. Palais 1.1 1
Chapter 1
Fiber Optic
Communications
Subject:Opto Electronics
Engr.Abid Hussain
Chohan
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Joseph C. Palais 1.1 2
Section 1.1
IntroductionHISTORY
Early communications used light signals.
Hand signals used light (from the sun or the moon)
as an information carrier.
The modulator was the hand of the sender.
The detector was the eye of the receiver.
The processor was the brain of the receiver.
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Joseph C. Palais 1.1 3
History
Early Optical Communications Smoke signals
Blinker lights
Photophone: invented by Alexander Graham Bell
Properties of early optical communications systems:
1) slow data rate
2) poor integrity, high error rate
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Joseph C. Palais 1.1 4
Modern Optical Communications
1960: The first laser was constructed.
1960-1970 Time Period:
Many laser applications were proposed.One proposal was for an optical
communications link that operated line-of-sight
though the atmosphere.
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Joseph C. Palais 1.1 5
Modern Optical Communications
Problems
A clear atmosphere was required for efficient
transmission.
The unguided atmospheric system needed an
unobstructed line-of-site.
Solution
In 1970, a low-loss, glass fiber waveguide was
developed at Corning.
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Joseph C. Palais 1.2 6
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Joseph C. Palais 1.2 7
Section 1.2
Basic Communications System
Transmitter
Information
ChannelReceiver
Messages are sent from the transmitter through
the information channel to the receiver.
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Joseph C. Palais 1.2 8
INFORMATION CHANNELS
Unguided Channels (Atmosphere)Radio Broadcast
Television Broadcast
Wireless
Satellite
Guided Channels
Conducting Wires
WaveguidesFibers
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Joseph C. Palais 1.2 9
INFORMATION CHANNELS
Applications For Guided Channels
Applications include:
cable television
telephone
data links [i.e., local area networks (LANs)]
The triple play:
Voice
Video
Data
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Joseph C. Palais 1.2 10
GENERAL OPTICAL SYSTEM
Message
Origin
Carrier
Source
Coupler
Modulator
Coupler
Detector
Processor
Destination
Optic
Domain
Electric Domain
Transmitter Receiver
Channel
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Joseph C. Palais 1.2 12
COMPONENTS OF A GENERAL
OPTICAL SYSTEMAnalog(continuous)
Time
Digital (discrete)
1 0 1 0 1
Time
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Joseph C. Palais 1.2 13
COMPONENTS OF A GENERAL
OPTIC SYSTEM
1.2.3 Carrier Source: Generates the lightwave
on which the informationis carried.
Common devices are:
laser diode (LD)
light emitting diode (LED)
The carrier source is intensity modulated. As theinput current changes, the output optical power
changes in the same way.
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Joseph C. Palais 1.2 14
COMPONENTS OF A GENERAL
OPTIC SYSTEMThe output power of the light source is proportional
to the input current.
Electrical Domain Optical DomainCarrier Source
ELECTRICAL
CURRENT, Iin
OPTICALPOWER, POUT
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Joseph C. Palais 1.2 15
GENERAL FIBER OPTIC SYSTEM
Intensity modulation: The transfer characteristics of
the ideal light source is
Optic
Power
(P)
Input current (I)
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Joseph C. Palais 1.2 16
GENERAL FIBER OPTIC SYSTEM
Example:
0 0 tt
I P
The above graphs indicate that the optic
power is directly proportional to the input
current.
Input
Current
Output
Optical Power
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Joseph C. Palais 1.2 17
GENERAL FIBER OPTIC SYSTEM
1.2.4 Coupler: Couples light from the source to the
fiber channel. The efficiency may not be high.
Why?
Answer:
1) Fibers are small (50 m diameters or less forsome fibers).
2) The fiber acceptance angle is small.
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Joseph C. Palais 1.2 18
GENERAL FIBER OPTIC SYSTEM
Light
Source
Fiber
Acceptance
angle
Light ray
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Joseph C. Palais 1.2 19
GENERAL FIBER OPTIC SYSTEM
1.2.5 Information channel: Glass (or plastic)
fibers that are the transmission medium.
Desirable properties:
1) Low attenuation (losses limit path lengths)
2) Low pulse (waveform) distortion
Pulses spread out as they propagate down the
fiber as indicated on the next slide.
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Joseph C. Palais 1.2 20
GENERAL FIBER OPTIC SYSTEMPulse Distortion (Pulse Spread)
Input
Power
Waveform after a short travel distance
Waveform after further travel
t
t
t
Power
Power
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Joseph C. Palais 1.2 21
GENERAL FIBER OPTIC SYSTEM
Solution to pulse spreading:
The pulses need to be spread out more at the
transmitter, so they do not overlap with each other
at the receiver. This means sending fewer pulses
per second. That is, transmitting at a lower data
rate.
Conclusion: Distortion limits the allowed data rate.
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Joseph C. Palais 1.2 22
GENERAL FIBER OPTIC SYSTEM
Receiver Coupler: Transfers the optic power
from the fiber to the photodetector.
Fiber
Photodetector
Electric
CurrentOptic Power
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Joseph C. Palais 1.2 23
GENERAL FIBER OPTIC SYSTEM
1.2.6 Photodetector: Converts optical power
to electric current. Ideally, the current is a
replica of the current used to modulate the
light source.
Optical Power
(Pin)
Electric
Current(Iout)
Photodetector
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Joseph C. Palais 1.2 24
GENERAL FIBER OPTIC SYSTEM
Transfer Characteristic for Photodetector
Optic Power (P)
Outputcurrent
(i)
Output current is
proportional to the
input optical
power.
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Joseph C. Palais 1.2 25
GENERAL FIBER OPTIC SYSTEM
Processing: Electrical domain processing consists
of the following.
1.2.7 Signal Processing
1) Amplification
2) Filtering to improve signal quality
3) Decision making circuitry for digital signals
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Joseph C. Palais 1.2 26
GENERAL FIBER OPTIC SYSTEM
Signal Quality Measures
Signal to noise ratio - measure for analog signals
Bit error rate - measure for digital
1.2.8 Message Destination
Devices such as output speakers, telephone
sets, video monitors, and computers.
1.2.9 Some Numbers
Important number in fiber optics
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Joseph C. Palais 1.2 27
Common UnitsTable
Units Symbol Measure
meter m lengthKilogram kg massSecond s timeCoulomb C chargeJoule J energy
Watt W power Hertz Hz frequencyNewton N ForceAmpere A CurrentKelvin K Temperature
Celsius C
TemperatureFarad F CapacitanceOhm ResistanceVolt V VoltageRadian r Angle
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Joseph C. Palais 1.2 28
IMPORTANT CONSTANTS
Description Value Symbol
Velocity of light 3*108m/s c
Planck constant 6.626*10-34J*s h
Electron charge -1.6*10-19 C -e
Boltzmann constant 1.38*10-23 J/K k
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Joseph C. Palais 1.2 29
PREFIXES
Prefix Symbol Multiplication Factor
tera T 1012
giga G 109
mega M 106
kilo k 103
centi c 10-2
milli m 10-3
micro 10-6nano n 10
-9
pico p 10-12
femto f 10-15
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Joseph C. Palais 1.2 30
COMMON UNITS IN FIBER OPTICS
Common units for calculation involving
lengths are:
nanometermn1m9
10
micronormicrometerm1m610
Optical wavelengths are usually in the above units.
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Joseph C. Palais 1.2 31
Bandwidths Of Common Systems
Common Analog Systems
Type Bandwidth CommentsVoice 4 kHz Telephone
Music 10 kHz AM radio broadcast
Music
TV
200 kHz
6 MHz
FM radio broadcast
Television broadcast
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Joseph C. Palais 1.2 32
Bandwidths Of Common Systems
Common Digital Systems
Type BW Comments
Voice 64 kbps Telephone
Ethernet 10 Mbps Xerox LAN
FDDI 100 Mbps Fiber distributed datainterface
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Joseph C. Palais 1.2 34
DIGITIZING VOICE MESSAGES
One 8-bit number consists of 8 time slots, each
containing a binary 0 or 1. There are 256 possible
combinations, since 28
= 256. Thus, a sequenceof 8 bits (combinations of zeroes and ones) will
represent the amplitude of each sample.
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Joseph C. Palais 1.2 35
DIGITIZING VOICE MESSAGES
Calculate the data rate:
8000(samples/s) x 8 (bits/sample) = 64,000 b/s
Therefore, there are 64,000 b/s transmitted for a
digitized voice message.
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Joseph C. Palais 1.2 36
MULTIPLEXING
We can mult ip lexnumerous messages by
transmitting at high transmission rates and
interleaving the bits from separate messages.
This is referred to as t ime div is ion mu lt ip lex ing
(TDM). The messages share the transmission
line. The receiver separates the individual
messages.
The field commander was here
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Joseph C. Palais 1.2 37
MULTIPLEXING
Examples of time division multiplexing.
Example 1: The T1 transmission level
operates at a standard rate = 1.544 Mb/s. Since
61.544 10
24.0664,000
Thus, 24 voice channels can be simultaneously
transmitted along a T1 transmission line.
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Joseph C. Palais 1.2 38
DIGITIZING VOICE SIGNALS
Examples of time division multiplexing.
Example 2: The T3 transmission level
operates at a standard rate = 44.7 Mb/s.
A T3 transmission normally carries up to 672
voice channels.
44.7x106/64,000 = 698
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Joseph C. Palais 1.2 39
ANALOG SIGNAL QUALITY
A measure of the quality of an analog signal is
the signal-to-noise ratio (SNR). It is the signal
power divided by the noise power.
S/N = (Signal Power)/(Noise Power)
For analog television signals, SNR > 10,000 is
required for decent viewing.
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Joseph C. Palais 1.2 40
DIGITAL SIGNAL QUALITY
The measure of quality for a digital system is the
bit error rate (BER). The BER is the fraction of
errors contained in a signal.
Example: A BER = 10-9means that there is one
error for every 109bits.
Digital systems require good bit error rates.
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Joseph C. Palais 1.2 41
1.2.10 Computing Power Levels in Decibels
The decibel scale is useful for analysis and design
of fiber components and systems.
P1
P2
Component
(System)
210
1
10log P
dBP
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Joseph C. Palais 1.2 42
THE DECIBEL SCALE
210
1
10log PdBP
This equation represents the decibel gain or loss
of the component (system). If there is loss the
decibel level will be negative, but if there is gain
then the decibel level will be positive.
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Joseph C. Palais 1.2 43
DECIBEL SCALE
The decibel scale is used to compare the ratio of
two power levels.
Example: Suppose P2/P1= 0.5. Then
dB = 10 log (0.5) = -3 dBExample: If P2/P1= 1, then
dB = 10 log 1 = 0 dB
Example: If P2/P1> 1, then dB is positiveExample: If P2/P1< 1, then dB is negative
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Joseph C. Palais 1.2 44
DECIBEL SCALE FOR CASCADED
ELEMENTS
The dB scale is useful for analyzing a system of
cascaded elements.
P1P
4
Element1 Element 2 Element 3
1
2
2
3
3
4
1
4
P
P
P
P
P
P
P
P P2 P3
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Joseph C. Palais 1.2 45
DECIBEL SCALE FOR CASCADED
ELEMENTS
Thus
123
1
210
2
310
3
410
1
2
2
3
3
410
1
410
log10log10log10
log10log10
dBdBdBdB
P
P
P
P
P
PdB
P
P
P
P
P
P
P
PdB
system
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Joseph C. Palais 1.2 46
DECIBEL SCALE FOR CASCADED
ELEMENTS
The dB of the cascaded elements are simply
added together. This illustrates the great
advantage of the decibel scale.
If the element has a loss, a negative sign
is placed in front of the dB value in the
preceding equation.
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Joseph C. Palais 1.2 47
DECIBEL ABSOLUTE POWER
SCALE
The decibel scale can be used to denote absolute
power if a reference power is specified. If the
reference power is set to 1 mW, we have the dBm
scale defined by
dBm = 10 log P
where P is in milliwatts. This is read as dB relativeto a milliwatt.
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Joseph C. Palais 1.2 48
DECIBEL ABSOLUTE POWER
SCALE
Example: If P = 2 mW, then
dBm = 10 log 2 = 3 dBm
Signs on the result are important. The dBm for
powers above one milliwatt (P > 1) will be
positive. The dBm for powers below a milliwatt
(P < 1) will be negative.
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Joseph C. Palais 1.2 49
DECIBEL ABSOLUTE POWER
SCALEThe dBscale is defined as:
dB= 10 log Pwhere P is in microwatts. This is read as dB
relative to a microwatt.
DECIBEL ABSOLUTE POWER
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Joseph C. Palais 1.2 50
DECIBEL ABSOLUTE POWER
SCALE
dBm1 dBm2
dBm2= dBm
1+ dB
x
210 10 2 10 1
1
2 1
2 1
10log 10log 10log
,
x x
x
x
PdB dB P P
P
dB dBm dBm
dBm dBm dB
Proof
dBxP1 P2
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Joseph C. Palais 1.2 51
Section 1 3
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Joseph C. Palais 1.3 52
Section 1.3
Wave Nature of LightSometimes light behaves as a wave and sometimes
light behaves as a particle. We will look at both
behaviors.
1.3.1 Wave Nature of Light
Light is an electromagnetic wave that satisfies
Maxwells Equations.
The electromagnetic spectrum is a range offrequencies classified into groups.
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Joseph C. Palais 1.3 53
Wave Nature of Light
1016 1015 1014 1013 1012 1011 1010 109 108 107 106 105 104 103 102 101 1
Ultraviolet
Visible
InfraredMillimeterwaves
Microwaves
Radio
Power
Frequency (Hz)
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Joseph C. Palais 1.3 54
WAVE NATURE OF LIGHT
Most of the frequencies in fiber optic systems are
In the Infrared.
Wavelength and frequency are related by:
f
vwherevis the velocity of the wave in the medium.
In free space,
v = c= 3 x108 m/s
(1.3)
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Joseph C. Palais 1.3 55
WAVE NATURE OF LIGHT
All materials slow down the light waves, so v < c in
all materials. If the material is changed, then the
wave velocity changes along with the wavelength.
The frequency remains constant, only the velocity
and the wavelength will change.
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Joseph C. Palais 1.3 56
WAVE NATURE OF LIGHTMost fiber optic communications systems operate
in the infrared region of the spectrum.
0.2 0.3 0.4 0.5 0.6 0.7 1.0 1.5 2.0
Wavelength (m)
Ultraviolet Visible Infrared
Optical Spectrum (Partial)
Blue Red
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Joseph C. Palais 1.3 57
WAVE NATURE OF LIGHT
Example: If is 0.85 m, find the frequency. Inthis example the medium is not specified, so let
us assume that the medium is free space.
814
6
3 10 /3.53 10
0.85 10
c m sf Hz
m
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Joseph C. Palais 1.3 58
WAVE NATURE OF LIGHT
The per iod o f osc i l lat ionT is defined as the time
it takes for the wave to complete one cycle. The
period for the frequency in the preceding
example is then
14
14
1 1
0.28 103.53 10T sf Hz
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Joseph C. Palais 1.3 59
WAVE NATURE OF LIGHTFiber optic systems must have low loss. For
glass low loss occurs at several wavelengths.
The major operation regions (w indows)are:
Wavelength Window
0.8-0.9 m First Window~1.300 m Second Window~1.550 m Third Window~1.600 m Fourth Window
These are all in the infrared.
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Joseph C. Palais 1.3 60
1.3.2 Particle Nature of Light
Light is made up particles called photons. Each
photon has energy:
p
c
W hf h h= 6.626 x 10-34J s (Plancks constant)
Shorter wavelength (higher frequency) waves have
greater photon energy.
(1.4)
PARTICLE NATURE OF
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Joseph C. Palais 1.3 61
PARTICLE NATURE OF
LIGHTExample: How many photons are delivered eachsecond for a wave with average power P = 1Wat wavelength = 0.8 m?The solution appears on the next slide.
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Joseph C. Palais 1.3 62
PARTICLE NATURE OF LIGHT
8
34
6
19
6 6
612
19
3 106.626 10
0.8 10
2.48 10
10 1 10
104.03 10
2.48 10
p
p
p
mc sW h J sm
JW
photon
W Pt Joules
W Jphotons
JW
photon
The photon energy is:
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C O G
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Joseph C. Palais 1.3 64
PARTICLE NATURE OF LIGHT
The electron volt (eV) is another useful unit for
analysis of fiber optic systems. The electron volt
is defined as the energy acquired by an electron
accelerated across a 1 volt potential difference.
The particle nature of light is used in explaining
the light sources and light detector later in the
text.
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Joseph C. Palais 1.2 65
Section 1 4
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Joseph C. Palais 1.4 66
Section 1.4
Advantages of Glass Fibers
Cost: The cost of fiber is very low, because glass is plentiful
and cheap.
Weight: Fiber cables are smaller than conducting cables
and weigh much less.
Strength: Fibers are strong and flexible, enabling them to go
around corners. Glass fibers have a very high tensile
strength.
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Joseph C. Palais 1.4 67
ADVANTAGES OF GLASS FIBERS
High informatioHigh information
capacity: Glass fiber can carry
more signals then a conducting
cable.
G S O G SS S
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Joseph C. Palais 1.4 68
ADVANTAGES OF GLASS FIBERS
Low Loss: As the modulation frequency
increases, coaxial cable losses increase at a
faster rate than do fiber losses.
Copper Fiberer
dB
loss(1kmleng
th)
Modulation Frequency(Hz)
4
73 dB
f 3-dB
3 dB OPTICAL BANDWIDTH
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Joseph C. Palais 1.4 69
3-dB OPTICAL BANDWIDTH
As light propagates down a fiber at low modulation
frequencies, its loss remains constant. At higher
modulation frequencies the signal power begins to
decrease.
The 3-dB opt ical bandwid this the frequency at
which the optical signal power is reduced by one
half. It is illustrated on the previous slide.
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Joseph C. Palais 1.4 70
0 1 2 3 4 5 6 70
0.5
1
1.5
2
2.5
3
3.5
4
time
opticalpowe
r
The 3dB
optical bandwidth
fa
f3-dB
is half the frequency and magnitude of fa
Average power
fc
OPTICAL 3-dB BANDWIDTH
fa
f3-dB
fc
TIME
OPTICALPOWER
OPTICAL 3 dB BANDWIDTH
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Joseph C. Palais 1.4 71
OPTICAL 3-dB BANDWIDTH
The previous slide illustrates the 3-dB optical bandwidth.
cd Ba fff 3
The signal attenuation is caused by the spreading of the
wave (pulse spreading) as it propagates down the fiber,
resulting in a lower peak power.
COMPARISON OF A FIBER CABLE
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Joseph C. Palais 1.4 72
COMPARISON OF A FIBER CABLE
WITH A WIRE CABLE
A wire cable consisting of 900 twisted pairs has adiameter of 70 mm. Each wire pair carries 24 voice
channels. The cable capacity is then:
24 x 900 = 21,600 voice calls
Compare this capacity to that of a T3 fiber cable containing
144 fibers having a diameter of 12.7 mm. At the T3 rate there
are 672 voice channels per fiber.
COMPARISON OF A FIBER CABLE
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Joseph C. Palais 1.4 73
COMPARISON OF A FIBER CABLE
WITH A WIRE CABLE
The fiber cable has total capacity:
672 x 144 = 96,768 voice calls
This is 4.5 times the capacity of the wire cable. In addition,
the fiber cross sectional area is 1/30th that of a wire cable.
The represents a great savings in space required for
installation.
ADVANTAGES OF FIBERS
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Joseph C. Palais 1.4 74
ADVANTAGES OF FIBERS
A. Fibers are insulators as opposed to conducting wires.
1) No current
2) No radiation from the sides of the fiber
3) No coupling between adjacent fibers
ADVANTAGES OF FIBERS
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Joseph C. Palais 1.3 75
ADVANTAGES OF FIBERS
B. Fibers reject interference. The following forms of
interference have no affect on fiber systems.
1) RFI: radio frequency interference from TV, radio, radar,
or other electronic signals.
2) EMI: electromagnetic interference from lighting,
sparking, or electromagnetic radiation.
3) EMP: electromagnetic pulse due to nuclear events.
ADVANTAGES OF FIBERS
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Joseph C. Palais 1.4 76
ADVANTAGES OF FIBERS
C. Fibers can be used near high power transmission
lines because of their insulation properties,
whereas wire systems would pick up a large amount
of noise.
D. Security: Fiber systems are difficult to tap.
E. Compatibility: Fibers are compatible with
conventional electronics.
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Joseph C. Palais 1.4 77
ADVANTAGES OF FIBERS
F. Corrosion resistant: Fiber, as opposed to wire systems,
resist corrosion.
G. Large temperature range: Glass melts at high
temperatures.
Section 1.5
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Joseph C. Palais 1.5 78
Applications of Fiber Systems1) Cable TV: Frequency-division-multiplexing (FDM) is
used to transmit television signals over fiber systems. Each
television channel has a bandwidth of 6 MHz.
Po
wer
0 f (Hz)6 MHz
TV Baseband Signal
FREQUENCY DIVISION
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Joseph C. Palais 1.5 79
MULTIPLEXING
Power
0 f (Hz)
6 MHz
TV Channel
fo
The television signal can be modulated onto a sub-
carrier frequency fo. The baseband signal has been
shifted upwards in frequency.
sub-carrier
FREQUENCY DIVISION
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Joseph C. Palais 1.5 80
MULTIPLEXING (FDM)
Electrical
0 f (Hz)
6 MHz
1
f1
Several television channels can be multiplexed onto different
sub-carrier frequencies and the result used to modulate a
light source.
f3f2 f4
6 MHz 6 MHz 6 MHz
2 3 4
Sub-Carrier Frequencies
Channels
FREQUENCY DIVISION
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Joseph C. Palais 1.5 81
MULTIPLEXING (FDM)
At the receiver the television signals are
demultiplexed by filters. Several tens of television
channels can be transmitted by frequency-
division-multiplexing (FDM) on a single fiber.
APPLICATIONS OF FIBER SYSTEMS
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Joseph C. Palais 1.5 82
APPLICATIONS OF FIBER SYSTEMS
2) Telephone trunk lines: In 1976-77 large-scale
fiber lines were first deployed to connect telephone
exchanges at 45 Mb/s. Fiber data rates are now
beyond 10 Gb/s.
3) Transatlantic cables: In 1989 transatlantic
cables were introduced that could handle 40,000
voice calls. Now all the major oceans and seas have
fiber cables lying beneath them.
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APPLICATIONS OF FIBER
SYSTEMS
4) Wired city: Due to increased demand, fiber-to-
the-home and fiber-to-the-curb systems are
available to bring higher data rates for video and
internet applications to businesses and to the
home.
5) Communications along electric railways: Fibersare not affected by electrical interference from the
railways.
APPLICATIONS OF FIBER SYSTEMS
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APPLICATIONS OF FIBER SYSTEMS
6) Communications along high voltage lines: Fibers
are not affected by interference from these lines.
7) Other video applications such as remote
monitoring and surveillance.
8) Local area networks (LANs), computers, file
systems: e.g., Ethernet.
9) Military applications such as tactical command
post telecommunications and fiber-guided
missiles.
APPLICATIONS OF FIBER SYSTEMS
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APPLICATIONS OF FIBER SYSTEMS
Sensors: Measurements of temperature, pressure, velocity,
motion and more.
The following is an example for a hydrophone sound
sensor.
Fluid
Fixed Fiber
Light Source Detector
speaker
sound wave
MonitorFree Fiber
APPLICATIONS OF FIBER SYSTEMS
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APPLICATIONS OF FIBER SYSTEMS
The hydrophone works on the principle of externalmodulation. The light is modulated by motion of
the fibers, causing misalignments in the
transmission system, resulting in a change inpower received.
S ti 1 6
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Section 1.6
Summary and Discussion
DECISIONS FACED BY DESIGNERS
Fiber or metal cable
Full-duplex or half-duplex two-way communications
Modulation format (analog or digital)
Multiplexing schemes
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Summary and Discussion
Wavelength of operation
Type of light source
Type of fiber
Choice of all other components