Title: TCOM 503 Fiber Optic Networks
1TCOM 503 Fiber Optic Networks
- Spring, 2007
- Thomas B. Fowler, Sc.D.
- Senior Principal Engineer
- Mitretek Systems
2Topics for TCOM 503
- Week 1 Overview of fiber optic communications
- Week 2 Brief discussion of physics behind fiber
optics - Week 3 Light sources for fiber optic networks
- Week 4 Fiber optic components fabrication and
use - Week 5 Fiber optic components, modulation of
light - Week 6 Optical fiber fabrication and testing of
components - Week 7 Noise and detection
3Topics for final exam (revised)
- Principles of fiber optic cable and devices
(reflection, refraction, interference,
diffraction) - Types of fiber optic cable
- Types of distortion and other problems involved
with optical fiber - Operation of LEDs and lasers
- Operation of detectors
- Operation of EDFAs
- Resonant couplers/wavelength selective couplers
splitters - Other optical devices
- Isolators - Fabry-Perot filters
- GRINs - Dielectric filters
- FBGs - Modulators Modulation types
- Optical fiber construction, fabrication
- Optical test instruments and how to interpret
their displays
4Optical fiber standard dimensions
- Core, cladding, jacketing standardized
- Jacket 245 mm
Source Corning
5Requirements for fabricating useful optical fiber
- Materials must be extremely pure
- Impurity lt 1 part per billion for metals
- Impurity lt 1 part per 10 million for water
- About 1000 times more pure than traditional
chemical purification techniques allow - Dimensions must be controlled to extremely high
degree - Core size, position, cladding size tolerances 1
micron or less - Roughly 1 wavelength of light
- Refractive indices must also be very precisely
controlled - Must be made in long lengths
- Must have tensile strength
6Purification of silica a two step process
- First use distillation
- Heat silica to boiling point (2230o C), condense
gas - Metals are heavier and do not boil at this
temperature - Yields impurity levels of 10-6
- Second stage takes place when fiber fabricated
7Fiber fabrication process
- Called Outside Vapor Deposition Process or OVD
process - Stages
- Laydown
- Consolidation
- Drawing
8First stage Laydown
- Vapor deposition from ultrapure vapors
- Soot preform made when vapors exposed to burner
and form fine soot particles of silica and
germanium
(From particles of silica and germania)
Source Corning
9Laydown (continued)
- Particles deposited on surface of rotating bait
rod - Core first
- Then silica cladding
- Vapor deposition process purifies fiber material
as impurities do not deposit as rapidly - Preform is somewhat porous at this stage
10Second stage consolidation
- Bait rod removed
- Placed in high-temperature consolidation furnace
- Water vapor removed
- Preform sintered into solid, dense, transparent
glass - Has same cross-section profile as final fiber,
but is much larger (1-2.5 cm, final 125 mm
.0125 cm)
11Third stage drawing
- Done in draw tower
- Glass blank from consolidation stage lowered into
draw furnace - Tip heated until gob of glass falls
- Pulls behind it a thin strand of glass
- Gob cut off
- Strand threaded into computer-controlled tractor
assembly - Sensors control speed of drawing to make precise
diameter
1850-2000o C
Source Corning
12Drawing (continued)
- Diameter measured hundreds of times per second
- Ensures precise outside dimension
- Primary and secondary coatings (jackets) applied
- At end, fiber wound onto spools for further
processing
Gob forming, Source Corning
13Draw tower
Source Axsys
14Other methods used to make fiber
- Vapor phase axial deposition (VAD)
- Batch process
- Preforms can be drawn up to 250 km
- Flame hydrolysis
- Soot formed and deposited by torches
15VAD process (continued)
Source Dutton
16Other methods used to make fiber (continued)
- Modified chemical vapor deposition (MCVD)
- Silica formed inside silica tube in gaseous phase
reaction - Soot deposited on inside of tube
- Burners traverse tube
- Sinters soot
- Produces highly controllable RI profile
- At end, tube evacuated, sides collapse
17MCVD process
Source Fotec
18Types of optical fiber
- Single mode glasslong distance communications
- Multimode glassshort distance communications
- Plasticconsumer short distance, electronics
cars - Hybrid or polymer clad (glass core, plastic
cladding)lighting, consumer applications
19Basic structure of all optical fiber
- Corecarries most of light
- Claddingconfines light to core
- In some fibers, substrate glass layer to add
strength - Inner jacket or primary buffer coatingmechanical
protection - Outer jacket or secondary buffer
coatingmechanical protection
Source Optical Cable Corporation
20Plastic optical fiber (POF)
- 1000 mm diameter, 980 mm core
- Strong
- Uses LEDs in visible range, 650 nm
- Not suitable for long-distance uses
- Does not transmit infrared
Source Pofeska/Mitsubishi Rayon Co.
21Numerical aperture
- Light must fall at an angle such that it can
enter fiber core, before total internal
reflection takes over - This angle is called numerical aperture
- www.corning.com/opticalfiber/discovery_center/tuto
rials/fiber_101/aperture.asp
22Basic cable construction types
- Tight buffered
- No room for fibers to move inside of cable
- Loose tube
- Multiple fibers loose inside of outer plastic
tube - Advantage is that with extra length of fiber
inside tube due to curling, less likelihood of
damage in sharp bends - Loose tube with gel filler
- Multiple fibers immersed in gel inside of plastic
tube
Source Dutton
23Typical indoor cable
- Single core or double core
- Utilize substrate for additional strength (aramid
or fiberglass)
Source Dutton
24Tight buffered indoor cable
- Application building risers
- 6 or 12 fibers typically
- Central strength member supports weight of cable
- Tight buffering means that fibers are not put
under tension due to their own weight
Source Dutton
25Outdoor cable
- More rugged, larger number of fibers per cable
- 6 fibers/tube, 6 tubes 36 fibers
- 8 fibers/tube, 12 tubes 96 fibers
- Steel or plastic used for strength member
- Outer nylon layer in locations where termites are
a problem
Source Dutton
26Outdoor cable (continued)
Source Dutton
27Submarine cable
- Smaller number of fibers because mechanical
requirements much greater - 4 to 20 typically
- Must withstand high pressure, damage from
anchors, trawlers, etc. - Cables for shallow water are in greatest danger
- Typically heavily armored
Source Dutton
28 MM 0.90/ftSM 0.53/ft
Indoor/OutdoorArmoredDirect bury
MM 6.65/ftSM 2.45/ft
Source Mohawk/CDT
29Splicing fiber geometry parameters
- Always necessary to splice fiber
- 3 parameters are most important to making good
splices - Cladding diameter tolerance
- Must be tight so that cores meet
- Typical spec is 125 mm 1.0 mm, removes this as
problem - Core/cladding concentricity
- Must be tight so that cores meet
- Fiber curl
- Must be minimal so that cores meet
30Fiber geometry parameters (continued)
31Cable connecting and splicing
- Problem of splicing and joining fibers
- Core is very small
- Any irregularity can lead to significant loss of
power or complete failure - Light is not like electricity
- Travels in waveguide and is a guided wave
- Requirements for good connection
- Precisely square cuts
- Ends polished flat
- Ends butted together
- Nearly exact matchup
32Ways of joining fibers
- Fusion splicing (welding)
- Commonly done in field
- Index matching epoxy glue
- Common done in field
- Mechanical connectors
- Used in field, but connectors attached in factory
- Not suitable for fiber breaks
33Dangers to fiber optic cable
- Excessive tension
- Bends of small radius
- Not generally problem with outdoor or undersea
cables because physical size keeps bend radius to
3 feet - Physical damage from animals, earth moving
equipment - Installation damage
- Lifting
- Pulling through conduits
- Water inflo
- Lightning
34Cabling environments
- Long-haul outdoor
- Usually direct bury
- Campus area outdoor
- Direct bury
- Conduit
- Outdoor overhead
- Undersea
- Most difficult environment
- Indoor
- Benign environment
- Installation usually most difficult problem
35Fusion splicing
- After cutting and polishing, ends are butted and
then fused by heat - Requires high temperature
- Can yield losses as low as 0.1 db (loss on 1 km
of fiber)
Source Dutton
36Steps in fusion splicing
- Strip primary coating on each fiber
- Cleave ends square
- Position ends a few mm from each other and clamp
- Align ends and bring closer together
- Electric arc started and melts glass, joining
fibers
37Problems with splicing
- When fiber ends melted and touched together,
surface tension effects tend to align outside of
cladding - Result is OK for multimode fibers with larger
cores - May not work for single mode fibers
- Single mode fibers require more precise alignment
- Use of laser shining into one fiber with detector
in the other - One fiber moved with precision actuator to
position it - Other problems can occur during join
- Surface tension can change fiber position as join
is made - Other systems use magnified image of fiber ends
displayed on a screen
38Problems with splicing (continued)
- Heating is difficult
- Best results when glasses melt and fuse
- Can change refractive index and hence cause
losses - Idea is to melt only a very thin layer on each end
39Joining with epoxy glue
- Ends cleaved and polished, space between them
filled with epoxy resin - Same RI as fiber core
- Fibers held in place mechanically
- Low cost but subject to many problems
- Concentricity
- Differing outside diameters
- Circularity of outside
- Tolerances of alignment device
- Long-term stability of epoxy
40Mechanical spicing and bonding
- Fibers inserted into silica sleeves
- Aligned as with welding method
- Bonded with epoxy
- High quality but costly
41Losses in fiber splices
- Extrinsiccaused by joining method but unrelated
to fiber properties - IntrinsicCaused by some inherent property of the
fiber
42Extrinsic losses
- Longitudinal misalignment
- Some light not within NA
- Endfaces form Fabry-Perot interferometer
- Lateral misalignment
- 2.5 microns 1 db loss
- Ends not square
- Surfaces cannot be joined closely
- Angular misalignment
- Losses due to NA
- 2o 1 db
- Fiber end rough or irregular
- Scattering
- No close contact
Source Dutton
43Intrinsic losses
- Concentricity
- Axes of core and fiber differ
- Greater for SM
- Core shape
- Not problem for MM
- For SM, causes fiber to be birefringent
- Different RIs for different polarizations
- Leads to PMD
- Core diameter
- Losses traveling from large to small diameter
- Cladding diameter
- If diameters differ, cores cannot be aligned
- NA and Refractive Index
- Some light reflected if these differ
Source Dutton
44Purely mechanical connectors
- Todays most common interconnection device
- Not fitted in field, as equipment expensive
(100K) and process difficult - Early connectors were poor
- Latest generation much better
- Components
- Ferrule long thin cylinder for alignment
- Connector body holds ferrule
- Cable attachment mechanism holds cable in body
- Coupling device where cables mate
- Fiber optic cables generally do not use
male/female connection method common for
electronic cables
45Purely mechanical connectors
Source Goff
46Connector evolution
Source Goff
47Commonly used fiber optic connectors
Source Goff Fotec
48 Source Goff Fotec
49Connectors (continued)
L to R SC-DC, LC, MT-RJ, SC, Volition, Opti-Jack
Source Fotec
50Fiber optic connector selection guide
51Typical data sheet
- hansonfiber.com/pdf/DS106320MTRJ.pdf
Source Johanson
52Typical fiber optic cable prices
- Indoor, multimode, duplex, with connector 50
0.50/ft - Outdoor, MM, 6 fibers/cable 0.90/ft
- Outdoor, MM, 96 fibers/cable 6.65/ft
- Outdoor, SM, 6 fibers/cable 0.53/ft
- Outdoor, SM, 96 fibers/cable 2.45/ft
- Submarine 65,000/km installed
53Testing of optical fiber
- Overview
- Standards
- Equipment
- Cable plant testing
- Network testing
54Overview of testing
- Definition process of verifying the performance
parameters of fiber optic components, links,
systems and networks and troubleshooting their
problems - Basic measurements
- Optical power emanating from a fiber
- Continuity or optical loss of fiber, cable,
connectors and splices - Bandwidth or dispersion
- Determines the information carrying capacity of
fiber or cable - Most tests must be repeated to determine changes
in measured parameters under environmental stress - Testing also includes finding problems in
installed fiber optic cable plants
55Tests and equipment
Test Equipment used
Optical power Fiber optic power meter
Attenuation or loss Fiber optic power meter source
Source wavelength, backscatter Optical loss test set, optical spectrum analyzer
Fault location Optical time domain reflectometer, visual cable fault locator
Bandwidth dispersion Bandwidth tester, simulation software
56Fiber optic power meters
- Measure average optical power emanating from
fiber - Basic components
- Detector (Si, Ga, or InGaAs)
- Signal conditioning circuitry
- Digital display
- Connectors for coupling to fiber
- Calibration
- Normal power units mw, microw, nw (linear scale)
- Power referenced to 1 mw or microw in db (dbm)
- Broad dynamic range (1 million to 1 or 60 db)
- Normal range of measurements 0 dbm to 50 dbm
57Fiber optic power meters (continued)
- Measurements require source with known duty
cycle, or knowledge of duty cycle of signal - Typically source has 2 kHz square wave output
- Uncertainty typically 5
58Typical optical power meter
59(No Transcript)
60Optical multimeter
Source Tektronix
61Fiber optic test source
- Standard signal source
- Compatible with type of fiber in use
- Single mode
- Multimode
- Wavelength
- Ability to connect to fiber and couple signal
- Same light source (LED or laser)
62Typical fiber optic test source
63Optical time domain reflectometer (OTDR)
- Uses phenomenon of fiber backscattering to
characterize fibers, find faults and optimize
splices - OTDR sends out into the fiber a high powered
pulse and measures the light scattered back
toward the instrument - Works since scattering is one of primary loss
factors in fiber (the other being absorption) - Pulse is attenuated on outbound leg and
backscattered light is attenuated on the return
leg - Returned signal is function of twice the fiber
loss and the backscatter coefficient of the fiber
64OTDR (continued)
- If one assumes the backscatter coefficient is
constant, OTDR can be used to measure loss - Gives a graphic display of status of fiber being
tested - Requires access to only one end of the fiber, as
opposed to both ends for power meters - Not a new device models exist for microwave
(CATV) and similar electronic applications
65Typical OTDR
66OTDR typical display
67OTDR specifications
68Tektronix OTDR
69Use of OTDRs
Pulse
Source Fotec
Backscattered light
70Operation of OTDRs
- Pulse from high-powered laser sent down fiber
- Pulse width 200 mm/ns
- Response measured on time scale
- Backscatter from pulse is what is sensed
- Longer distances require longer pulses
- Decreases accuracy
71OTDR trace
Reflection from first connector
Noise typically seen here
Source Fotec
72More OTDR traces
Source Fotec
73More OTDR traces
Source Fotec
74OTDR performance limitations
- Accuracy limited by several factors
- Pulse width
- Long pulse for long cables 100 ns or longer
- Short pulse for short cables 10 ns
- Speed of light variations among fibers
- 1-2 10-20 m/km
- Backscatter not constant between fibers
- Initial saturation means minimum distance
measurement 100 to 1000 m unless precautions
taken - Requires launch cable to allow transients to
die out - Long fibers resolution 250-500 m
- Short fibers 5-10 m
- Limited usefulness for in-building testing
75Signal analyzer
- Used to measure performance parameters of optical
systems - Q-factor
- Extinction ratio
- Optical power
- Signal-to-noise ratio
- Jitter
- Duty cycle
- Eye diagrams
- High-performance models directly calculate
parameters - Work on Return-to-zero (RZ) and
non-return-to-zero (NRZ) signals
76Typical high-performance signal analyzer
Source Tektronix
77Visual cable tracers and fault locators
- Many problems in connection of fiber optic
networks are related to making proper connections - Since light used in systems is invisible, one
cannot see the system transmitter light - By injecting light from a visible source, such as
a LED or incandescent bulb, one can visually
trace the fiber from transmitter to receiver - To insure correct orientation
- To check continuity
- Simple instruments that inject visible light are
called visual fault locators
78Typical fault tracers
Source Fotec
79Fiber optic inspection microscopes
- Inspecting connector finish during polishing
- Inspecting installed connectors for dirt or
scratches - Inspecting bare fiber before splicing.
- Assures only properly cleaved fibers are used for
splices
80Inspection microscope
Source Fotec
81Optical spectrum analyzer
- Shows graphically how power is distributed as
function of wavelength or frequency
Source Agilent
82Typical unit
Source Agilent 86140B www.agilent.com/cm/rdmfg/os
a/86140b/index.shtml
83Close up of trace
Source Agilent 86140B
84Controls
Source Agilent 86140B
85(No Transcript)
86(No Transcript)
87Typical traces from spectrum analyzer
EDFA
FP laser
Source Agilent
88Optical power in common communications
applications
Source Fotec
89Causes of error in fiber optic power measurement
- Imperfect optical coupling
- Reflection from coupled surfaces
- Dirt and other contaminants on optical surfaces
- Wavelength calibration
- Most meters are calibrated for particular
wavelength or set of wavelengths - Excessively high or low levels
- Exceed linear range of meter
- High levels saturation
- Low levels noise interference
- Field measurements typically made to 0.1 db
accuracy
Source Fotec
90Fiber types
Source Fotec
91Testing attenuation
- Basic setup
- Method
- Insert modal condition(if multimode fiber)
- Measure power at end
- Calculate
- If multimode, removeconditioner by cuttingback
and remeasure
Source Fotec
92Modal distribution problems
- In multimode fiber, strength of modes is function
of length - In single mode fiber, there is only one mode
- Zero order mode straight-through path
- Higher-order modes paths which bounce off of
cladding - Travel longer distance
- Experience more attenuation because path is
longer - Equilibrium modal distribution(EMD) refers to
modes in longfiber, where higher-order
modeslost through attenuation
Source Fotec
93Modal distribution problems (continued)
- Modal distribution depends on many factors
- Source
- Fiber
- Components encountered (splices, connectors,
etc.) - Accurate and reproducible measurement of power in
multimode fiber depends on knowing (or
standardizing) modal distribution - Also a function of type of coupling used
- Mode conditioners
- Strippers (remove unwanted cladding mode light)
- Scramblers (equalize power in modes)
- Filters (remove higher-order modes to simulate
long distances)
94Fiber mode distribution attenuation
Source Fotec
95Testing bandwidth and dispersion
- Modal dispersion
- Use narrow spectral width laser, high-speed
receiver - Modulate laser with sine waves (sweep generator)
- Measure attenuation
- Alternate method measure degradation of pulse
risetime - Chromatic dispersion
- Compare pulse transit times as function of
wavelength - Requires several different laser sources of
different wavelengths - Equipment needed is very expensive
96Fiber optic link performance parameters
Link type Source/Fiber Wave-
Transmit Receiver Margin
length (nm)
Power (dbm) Sensitivity (dbm) (dB)
Telecom laser/SM 1300
3 to -6 -40 to -45 34 to 48
1550
0 to 10 -40 to -45
40 to 45 Datacom LED/MM 850
-10 to 20 -30 to -35 10
to 25
1300 -10 to -20 -30 to -35
10 to 25 CATV(AM) laser/SM 1300
10 to 0 0 to -10
10 to 20
Source Fotec
97Fiber optic link testing and troubleshooting
- Use power source and meter to test end-to-end
power loss and power levels - If there is a problem, work back from receiver to
transmitter - Types of tests
98Fiber optic link testing and troubleshooting
(continued)
- Many systems and components can be tested with
loopback