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Fiber Characterization Assessing the fiber’s capacity Tim Yount Market Manager - Fiber Optic Test Solutions JDSU Fiber Optic Division
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Page 1: Ppt

Fiber Characterization Assessing the fiber’s capacity

Tim YountMarket Manager - Fiber Optic Test SolutionsJDSU Fiber Optic Division

Page 2: Ppt

© 2007 JDSU. All rights reserved. 2

Optical Communication Networks

There are a large variety of network topologies possible according to

distance reach, environments, bandwidth and transmission speeds.

Buildings

Multi-home Units

Residential

CO/Headend/

MTSO

Local Convergence Point

Network Access Points

High Speed DWDM network Access/FTTx network- HFC, RFoG, Docsis PON

Page 3: Ppt

Fiber Review

Singlemode Optical Fiber

Page 4: Ppt

NOT FOR USE OUTSIDE VERIZON AND JDSU

4

Light propagation is a function of Attenuation, dispersion and non-linearities.

Attenuation, Dispersion,

02

1

2

2

2

2

2

AAdT

AA

i

z

Ai

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© 2007 JDSU. All rights reserved. 5

Optical Transmission

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© 2007 JDSU. All rights reserved. 6

Optical Fiber Types

2 types:– Singlemode– Multimode

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© 2007 JDSU. All rights reserved. 7

Industry Standards

Industry Standards for Fiber (ITU)

For Multimode & Single Mode

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© 2007 JDSU. All rights reserved. 8

Elements of Loss

Pin (Emitted Power)

Pout

(Received power)

Power variation

Fiber Attenuation

Caused by scattering & absorption of light as it travels through the fiber

Measured as function of wavelength (dB/km)

OTDR Trace of a fiber link

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© 2007 JDSU. All rights reserved. 9

Bending Losses

Microbending – Microbending losses are due to

microscopic fiber deformations in the core-cladding interface caused by induced pressure on the glass

Macrobending – Macrobending losses are due to

physical bends in the fiber that are large in relation to fiber diameterAttenuation due to macrobending increases with wavelength (e.g. greater at 1550nm than at 1310nm)

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© 2007 JDSU. All rights reserved. 10

Optical Return Loss (ORL)

Amount of transmitted light reflected back to the source

PT: Output power of the light source

PAPC: Back-reflected power of APC connector

PPC: Back-reflected power of PC connector

PBS: Backscattered power of fiber

PR: Total amount of back-reflected power

ORL (dB) = 10.Log > 0)(R

T

P

P

PAPCPPC Pelement PAPC

PT

PBS PBS PBS

Source(Tx)

Receiver(Rx)

PR

ORL is measured in dB and is a positive value. The higher the number, the smaller the reflection - yielding the desired result.

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© 2007 JDSU. All rights reserved. 11

Effects of High ORL (Low values)

Increase in transmitter noise– Reducing the OSNR in analog video transmission– Increasing the BER in digital transmission systems

Increase in light source interference – Changes central wavelength and output power

Higher incidence of transmitter damage

The angle reduces the back-reflection of the connection.

SC - PC SC - APC

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© 2007 JDSU. All rights reserved. 12

Pulse Spreading

Chromatic Dispersion

Chromatic Dispersion (CD) is the effect that different wavelengths (colors or spectral components of light) travel at different speed in a media (Fiber for ex.)

The more variation in the velocity, the more the individual pulses spread which leads to overlapping.

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© 2007 JDSU. All rights reserved. 13

Dispersion Compensation

The Good News: CD is stable, predictable, and controllable– Dispersion zero point and slope obtained from manufacturer– Dispersion compensating fiber (“DC fiber”) has large negative

dispersion– DC fiber modules correct for chromatic dispersion in the link

Tx Rx

DC modulesfiber span

delay [ps]

0 d

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© 2007 JDSU. All rights reserved. 14

Standard SM fiber span

DGD

v1

v2

V1 > V2

Polarization Mode Dispersion

Different polarization modes travel at different velocities presenting a different propagation time between the two modes (PSPs).

The resulting difference in propagation time between polarization modes is called Differential Group Delay (DGD).

PMD is the average value of the Differential Group Delay (mean DGD), so called PMD delay [ps], expressed by the PMD delay coefficient c [ps/km]

Perfect SM Fiber span

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© 2007 JDSU. All rights reserved. 15

What are my PMD limitations ?

According to the theoretical limits or equipment manufacturers specs, determine the PMD delay [ps] margin.– PMD varies randomly so abs. value to be used with care.– Consider margin knowing “typical” variation (from the data) occur in a 10-20%

magnitude. What are my distance limitations due to PMD?

– PMD coefficient [ps/√km ] calculated

10 Gbit/s (OC-192)10 Gbit/s (OC-192)

40 Gbit/s (OC-76840 Gbit/s (OC-768

2.5 Gbit/s (OC-48)2.5 Gbit/s (OC-48) 6,400 km6,400 km

400 km400 km

25 km25 km

Max Distance @ 0.5ps√km

Birefringent sections (randomly concentrated)

DGD

v1

v2

External stress !!

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Connector Contamination

Understanding Contamination on Fiber Optic Connectors and Its Effect on Signal Performance

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© 2009 JDSU. All rights reserved. JDSU CONFIDENTIAL & PROPRIETARY INFORMATION17

Focused On the Connection

Fiber connectors are widely known as the WEAKEST AND MOST

PROBLEMATIC points in the fiber network.

Bulkhead Adapter

Fiber Connector

Alignment Sleeve

Alignment Sleeve

Physical Contact

FiberFerrule

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© 2009 JDSU. All rights reserved. JDSU CONFIDENTIAL & PROPRIETARY INFORMATION18

What Makes a GOOD Fiber Connection?

Perfect Core Alignment

Physical Contact

Pristine Connector Interface

The 3 basic principles that are critical to achieving an efficient fiber optic

connection are “The 3 P’s”:

Core

Cladding

CLEAN

Light Transmitted

Today’s connector design and production techniques have eliminated most of the challenges to achieving Core Alignment and Physical Contact.

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© 2007 JDSU. All rights reserved. 19

What Makes a BAD Fiber Connection?

A single particle mated into the core of a fiber can cause significant back reflection, insertion loss and even equipment damage.

Today’s connector design and production techniques have eliminated most of

the challenges to achieving CORE ALIGNMENT and PHYSICAL CONTACT.

What remains challenging is maintaining a PRISTINE END FACE. As a result,

CONTAMINATION is the #1 source of troubleshooting in optical networks.

DIRT

Core

Cladding

Back Reflection Insertion LossLight

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© 2007 JDSU. All rights reserved. 20

Illustration of Particle Migration

Each time the connectors are mated, particles around the core are displaced, causing them to migrate and spread across the fiber surface.

Particles larger than 5µ usually explode and multiply upon mating.

Large particles can create barriers (“air gaps”) that prevent physical contact.

Particles less than 5µ tend to embed into the fiber surface, creating pits and chips.

11.8µ

15.1µ

10.3µ

Actual fiber end face images of particle migration

Core

Cladding

Page 21: Ppt

Characterizing the Fiber Plant

Understanding Fiber Link and Network Characterization

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© 2007 JDSU. All rights reserved. 22

What is Fiber Characterization?

Fiber Characterization is simply the process of testing optical fibers to ensure that they are suitable for the type of transmission (ie, WDM, SONET, Ethernet) for which they will be used.

The type of transmission will dictate the measurement standards used

Trans type Speed PMD Max CD Max

SONET 10 Gbs 10 ps 1176ps/nm

Ethernet 10 Gbs 5 ps 738 ps/nm

SONET 40 Gbs 2.5 ps 64 ps/nm

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© 2007 JDSU. All rights reserved. 23

Link & Network Characterization

Link Characterization– It measures the fiber

performance and the quality of any interconnections

– The suite of tests mostly depend on the user’s methods and procedures

– It could be uni-directional or bi-directional

– Tests – Connector Inspection, IL, ORL, OTDR, PMD, CD, AP

Network Characterization– It provides the network baseline

measurements before turning the transmission system up.

– Network Characterization includes measurements through the optical amplifiers, dispersion compensators, and any elements in line.

– It is a limited suite of tests as compared to Link Characterization

Point BPoint A

CWDM/DWDM Optical Network

Optical Amp.Video Headend

DWDM

Optical

Network

ROADM

Optical AmplifierRouter

Page 24: Ppt

Testing the Fiber Plant Connector inspection Insertion Loss OTDR Optical Return Loss Polarization Mode Dispersion (PMD) Chromatic dispersion (CD) Attenuation profile (AP)

@ On@ Charge

LASERON/OFF

PREV

LEVELADJUST

MENUENTER

CW/FMOD

☼LASERON/OFF

PREV

LEVELADJUST

MENUENTER

CW/FMOD

☼☼

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© 2007 JDSU. All rights reserved. 25

Inspect Before You Connectsm

Follow this simple “INSPECT BEFORE YOU CONNECT” process to ensure fiber

end faces are clean prior to mating connectors.

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© 2007 JDSU. All rights reserved. 26

Inspect, Clean, Inspect, and Go!

Fiber inspection and cleaning are SIMPLE steps with immense benefits.

44 Connect

■ If the fiber is clean, CONNECT the connector.

NOTE: Be sure to inspect both sides (patch cord “male” and bulkhead “female”) of the fiber interconnect.

22 Clean

■ If the fiber is dirty, use a simple cleaning tool to CLEAN the fiber surface.

11 Inspect

■ Use a probe microscope to INSPECT the fiber.

– If the fiber is dirty, go to step 2, cleaning.

– If the fiber is clean, go to step 4, connect.

33 Inspect

■ Use a probe microscope to RE-INSPECT (confirm fiber is clean).

– If the fiber is still dirty, go back to step 2, cleaning.

– If the fiber is clean, go to step 4, connect.

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© 2007 JDSU. All rights reserved. 27

Measuring Insertion Loss

The insertion loss measurement over a complete link requires a calibrated source and a power meter.

This is a unidirectional measurement, however could be performed bi-directionally for operation purposes

Calibrated Light Source

dBm WMenu Ca

nc

el

dB

>2s

Perm

Optical power meter

d B mW d B

Pt Pr

This measurement is the most important test to be performed, as each combination of transmitter/receiver has a

power range limit.

It is the difference between the transmitted power and the received power at the each end of the link

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© 2007 JDSU. All rights reserved. 28

OCWR method

Measuring Optical Return Loss

Different methods available The 2 predominant test methods:

– Optical Continuous Wave Reflectometry (OCWR)• A laser source and a power meter, using the same test port, are

connected to the fiber under test.

– Optical Time Domain Reflectometry (OTDR)• The OTDR is able to measure not only the total ORL of the link but

also section ORL (cursor A – B)

OTDR method

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© 2007 JDSU. All rights reserved. 29

Optical Time Domain Reflectometer (OTDR)

OTDR depends on two types of phenomena:- Rayleigh scattering - Fresnel reflections.

Rayleigh scattering and backscattering effect in a fiber

Light reflection phenomenon = Fresnel reflection

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© 2007 JDSU. All rights reserved. 30

How does OTDR work ?

An Optical Time Domain Reflectometer (OTDR) operates as one-dimensional radar allowing for complete scan of the fiber from only one end.

The OTDR injects a short pulse of light into one end of the fiber and analyzes the backscatter and reflected signal coming back

The received signal is then plotted into a backscatter X/Y display in dB vs. distance

Event analysis is then performed in order to populate the table of results.

OTDR Block Diagram Example of an OTDR trace

Distance

Fiber under test

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© 2007 JDSU. All rights reserved. 31

Optical Time Domain Reflectometer (OTDR)

Detect, locate, and measure events at any location on the fiber link

Fusion Splice Connector ormechanical Splice

Gainer

• OTDR tests are often performed in both directions and the results are averaged, resulting in bi-directional event loss analysis.

• OTDRs most commonly operate at 1310, 1550 and 1625 nm singlemode wavelengths.

Macrobend Fiber end or break

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© 2007 JDSU. All rights reserved. 32

Contamination and Signal Performance

Fiber Contamination and Its Effect on Signal PerformanceCLEAN CONNECTION

Back Reflection = -67.5 dBTotal Loss = 0.250 dB

11

DIRTY CONNECTION

Back Reflection = -32.5 dBTotal Loss = 4.87 dB

33

Clean Connection vs. Dirty Connection

This OTDR trace illustrates a significant decrease in signal performance when dirty connectors are mated.

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© 2007 JDSU. All rights reserved. 33

ps

<10 secondsPMDLight

Source

Measuring PMD

Different PMD standards describing test methods • IEC 60793-1-48/ ITU-T G.650.2/ EIA/TIA Standard FOTP-XXX

The broadband source sends a polarized light which is analyzed by a spectrum analyzer after passing through a polarizer

PMDReceiver

The PMD measurement range should be compatible the transmission bit rate. In order to cover a broad range of field applications, it should be able to measure between 0.1 ps and 60 ps.

PMD measurement is typically performed unidirectional. When PMD results are too close to the system limits, it may be required to perform a long term measurement analysis in order to get a better picture of the variation over the time.

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© 2007 JDSU. All rights reserved. 34

Dealing with PMD

PMD constraints increase with:– Channel Bit rate– Fiber length (number of sections)– Number of channels (increase missing channel possibility)

PMD decreases with:– Better fiber manufacturing control (fiber geometry…)– PMD compensation modules.

PMD is more an issue for old G652 fibers (<1996) than newer fibers

At any given signal wavelength the PMD is an unstable phenomenon, unpredictable. So has

to be measured

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© 2007 JDSU. All rights reserved. 35

Measuring CD

There are different methods to measure the chromatic dispersion. IEC 60793-1-42 / ITU-T G650.1; EIA/TIA-455- FOTP-175B

The Phase Shift method is the most versatile one. It requires a source (broadband or narrow band) and a receiver (phase meter) to be connected to each end of the link

The Chromatic dispersion measurement will be performed over a given wavelength range and results will be correlated to the transmission system limits according to the bit rate being implemented.

Parameters to be controlled in such way to correlate to the equipment specifications:

– Total link dispersion.– Dispersion slope– Zero dispersion wavelength and

associated slope

CDLight

Source

CDReceiver

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© 2007 JDSU. All rights reserved. 36

Measuring AP

Every fiber presents varying levels of attenuation across the transmission spectrum. The purpose of the AP measurement is to represent the attenuation as a function of the wavelength.

A reference measurement of the source and fiber jumpers is required prior to performing the measurements.

The receiver records the attenuation per wavelength of the source used for transmission.

This could be used to determine amplifier locations and specifications, and could have an impact on channel equalization (macro or micro-bends).

Spectral attenuation measurements are typically performed unidirectional. The wavelength measurement range should be at least equivalent to transmission system: C-band or C+L band.

IEC 60793-1-1 Optical fibers – Part 1-1: Generic Specification – GeneralTest procedureITU-T G.650.1

C+L DWDM Band AP results

Water peak

BroadbandLight

Source

NarrowbandReceiver

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© 2007 JDSU. All rights reserved. 37

Fiber Characterization Results

Page 38: Ppt

Wrap Up

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© 2007 JDSU. All rights reserved. 39

The Tools for Installing & Maintaining NetworksFiber Links

Inspection & Cleaning

Loss/ ORL Test sets

OTDR

Dispersion testers (PMD and CD)

Attenuation Profile testers

Network / Transport

Inspection & Cleaning

Power Meters

Ethernet Testers

BER Testers

Optical Spectrum Analyzers

Network Characterization (System Total Dispersion)

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© 2007 JDSU. All rights reserved. 40

Q&A and Resources

Questions

Contacts

Name - Company (Title) Phone E-mail Fred Ingerson – 4th Wave (JDSU Mfg Rep) (315) 436-0895 [email protected]

Mark Leupold – JDSU (MSO Acct Mgr) (540) 226-6284 [email protected]

John Swienton – JDSU (FO App Specialist) (413)231-2077 [email protected]

Greg Lietaert – JDSU (FO Prod Line Mgr) (240) 404 2517 [email protected]

Tim Yount – JDSU (FO Test Mkt Mgr) (207)329-3342 [email protected]

For more on Fiber Characterization visit: www.jdsu.com/characterizationThere you’ll find…Technical Posters, White Papers, Quick Start Guides, FO Guidebooks, Product and Service Information, and more…