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May 2008 Cables-Engl -1 © P. Nicolet ti: see note pag. 2 Copper and Fiber Optic Cables Pietro Nicoletti piero[at]studioreti.it

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Page 1: Cables Engl

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May 2008

Cables-Engl - 1 © P. Nicoletti: see note pag. 2

Copper and Fiber Optic Cables

Pietro Nicolettipiero[at]studioreti.it

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May 2008

Cables-Engl - 2 © P. Nicoletti: see note pag. 2

Copyright note These slides are protected by copyright and international treaties. The title and the

copyrights concerning the slides (inclusive, but non only, every image, photograph,animation, video, audio, music and text) are the author’s (see Page 1) property.

The slides can be copied and used by research institutes, schools and universitiesaffiliated to the Ministry of Public Instruction and the Ministry of University andScientific Research and Technology, for institutional purpose, not for profit. In thiscase there is not requested any authorization.

Any other complete or partial use or reproduction (inclusive, but not only,reproduction on discs, networks and printers) is forbidden without written

authorization of the author in advance. The information contained in these slides are believed correct at the moment of

publication. They are supplied only for didactic purpose and not to be used forinstallation-projects, products, networks etc. However, there might be changeswithout notice. The authors are not responsible for the content of the slides.

In any case there can not be declared conformity with the information contained in

these slides. In any case this note of copyright may never be removed and must be written also

in case of partial use.

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Copper cables main characteristics The main characteristics of a transmission media are:

Vp: Velocity of propagation of the signal expressed as

c fraction (speed of the light in the empty space): values included between 0.5 and 0.8 c

Z = r+jI impedance of the line

conductors' dimension

american AWG unit of measurement

Diameter, electrical resistance

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AWG: American Wire Gage Scale to measure the copper wire dimension

It is a geometrical regression

with 39 values in the interval 000 gage (0.460 diameterinch) and 36 gage (0.005 diameter inch)

Every increase of a gage corresponds to a diameter

relationship of:

0.460

0.005( )

1/39

= 92 = 1.2293221/39

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Copper cables AWG

AWG mm (Ø) mm2 Kg/Km Ω /Km

22 0.6438 0.3255 2.894 52.96

23 0.5733 0.2582 1.820 84.21

24 0.5106 0.2047 1.746 87.82

25 0.4547 0.1624 1.414 108.4

26 0.4049 0.1288 1.145 133.9

24 or 22 AWG for structured cabling system

26 AWG for patch cord

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Copper cable attenuation The attenuation is the output signal reduction with

respect to the entry signal in the cable:

attenuation linearly grows in dB with the length of thecable and the frequency square root

to reduce the cable attenuation expanded insulators areused because improve the capacity

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Attenuation

V1 V2

αdB = 20 log10 (V1 / V2)

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Copper pair Cross-Talk Signal energy part induction on the near conductors,

where a disturb becomes

The phenomenon increases with increasing it byfrequency

It can be measured in several manners

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NEXT: Near End Cross-Talk Cross-Talk measured at the transmitter side

V1

V3

NEXTdB = 20 log10 (V1 / V3)

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NEXT: Near End Cross-Talk The attenuation only makes the NEXT measure

significant by the first 20-30 mt of cable

The measurement is necessary to both ends: dual NEXT

V1

V3

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FEXT: Far End Cross-Talk Cross-Talk measured at the receiver side

V1

V4

FEXTdB = 20 log10 (V1 / V4)

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ACR ACR (Attenuation to Cross-Talk Ratio)

Combination of attenuation and NEXT

signal to noise ratio

noise caused by Cross-Talk

Required only by ISO and EN normative

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ELFEXT: Equal Level FEXT

~

~

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PSELFEXT (Power Sum ELFEXT)

~~

~~

~~

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Velocity of propagation (Vp) The propagation velocity of the signals on the

transmission means is high, but not infinite, so the

propagation time is little but not null It is necessary to ensure that delays do not exceed

certain maximum values to ensure the protocol working

VP ≅ 2/3 c

( c

is speed of the light in the empty space ≅ 3 • 10 8 m/s)

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Delay skew

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Return loss Il return loss = reflections measurements

Z1 Z3Z2Impedancevariations

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Shielded cable The shield presence can involve:

bigger immunity to the electromagnetic disturb

disturb radio emission reduction

bigger constancy of the impedance

if applied to single pair reduces the crosstalk

It is necessary to make a correct screen grounding:

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Twisted pair cable Constituted by one or more twisted pair of copper

conductors

Used for voice, local nets, structured cabling system the electrical characteristic required for LAN are

definitely higher than those for voice

Lower bandwith than the coaxial one Reduced costs and simple installation

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Twisted Pair cable types UTP (Unshielded Twisted Pair):

(Z = 100 Ω)

FTP (Foiled Twisted Pair):

(Z = 100 Ω)

S-UTP o S-FTP:

(Z = 100 Ω) STP (Shielded Twisted Pair):

(Z = 150 Ω)

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UTP 100 Ω

pair 1

pair 2

pair 3

pair 4

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FTP 100 Ω

pair 1pair 2

pair 3

pair 4

Drain wire for shield continuity

Foil shield

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S-UTP or S-FTP 100 Ω

pair 1

pair 2

pair 3

pair 4

Copper braid

Single foil shielded pair

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STP 150 Ω Know as Type 1 IBM

22 AWG

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GLASS FIBER OPTIC

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Glass Fiber Optic It is a tiny and flexible glass material thread:

an internal part called core

an outside part called cladding core and cladding have different refraction indexes to

border the light inside core

CORE

CLADDING

PRIMARY COATING

SECONDARY COATING

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Glass Fiber Optic characteristics The optic fibers are just suitable for point point links

Total immunity to the electromagnetic troubles

Characterized by two numbers n/m where:

diameter n of the leading internal light part

diameter m of the outside part

Typical values in micronmultimode 50/125, 62.5/125, 100/140

singlemode 8-10/125

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Step-index multimode fiber Characteristics

High modal dispersion

Low bandwith

M1

M4M3

M2

M1

M2

M3

M4

T1 T2

Input signal Output signal

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Graded-index multimode fiber Graded-index fiber have a bandwith higher than step-

index

work in 1st and 2nd window (850 and 1300 nm)

M 2008

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Singlemode fiber

The fiber behaves like a wave guide admitting asingle propagation mode:

does not have modal dispersion

the bandwith is very high, of the order of hundredsof GHz*Km

work in 2nd

and 3th

window (1300 and 1500 nm)

May 2008

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Wavelenght and optical components

A t t e n u a

t i o n ( d B X K m

)100

1

5

10

500 600 700 850 900 1000 1100 1200 13001310

1400 1550

LED\VCSEL

LASER DIODEVCSEL

LASER DIODE

May 2008

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Fiber optic cable types Tight

Break-out

dual fiber patch cord Light-duty

Loose

May 2008

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Break-Out tight fiber optic cable

Fiber opticExternal diameter 250 µm

250 µm = 125 µm + primary coating

CentralDielectric element

SheathToxfree or Low-smoke-fume

Kevlar

Secondary coatingExternal diameter 0.9 mm

External diameter 2 ÷ 3 mm

Indoor installation

May 2008

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Dual fiber patch cord

Fiber opticExternal diameter 250 µm

250 µm = 125 µm + primary coating

SheathToxfree o Low-smoke-fume

Kevlar

Secondary coatingExternal diameter 0.9 mm External diameter 2 ÷ 3 mm

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Light-duty tight fiber optic cable

CentralDielectric element

Kevlar

Secondary coatingExternal diameter 0.9 mm

Fiber opticExternal diameter 250 µm

250 µm = 125 µm + primary coating

Roditor resistant protection

SheathToxfree o Low-smoke-fume

Indoor/Outdoor installation

May 2008

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Loose fiber optic cable

Fiber optic

External diameter 250 µm250 µm = 125 µm + primary coating

CentralDielectric element

Kevlar

Roditor resistant protection

TubeJelly filled

Sheath

Sheath

Outdoor installation