(159373063) design of a low impedance grounding system for telecom applications - mitchell guthrie...

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  • 8/12/2019 (159373063) Design of a Low Impedance Grounding System for Telecom Applications - Mitchell Guthrie and Alain Rousseau

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    A li ti

    Designof a Low Impedance

    Mitchell GuthrieIndependent Engineering Consultant

    Alain RousseauSEFTIM

    Grounding System for Telecom

    Applications

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    Relate gro nding s stem impedance to

    Objectives

    Discuss impedance performance criteria

    Discuss typical existing performance

    criteria

    Discuss relationship between resistance

    and impedance

    Identify broadband response of grounding

    system components and systems

    Relate grounding system impedance to

    telecom applications

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    f di i t d

    ImpulseCurrentEffects

    in the earthing

    Low frequency contentenergy zone

    V(t) = i(t) R + L (di/dt)

    High frequency

    content is important

    for overvoltages

    Low frequency

    content is important

    High frequency contentfor energy dissipated

    sparkover zone system

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    ImpulseCurrentPrinciples

    earth

    can result

    into earth as a function of earth resistivity or conductors

    earth decreases current density at earth / electrode

    Lightning takes the lowest impedance path to remote

    lowest resistance and lowest inductance paths preferred

    High inductance path leads to high voltage on LPS current cannot change instantaneously through an inductance

    overvoltage is created and spark over to a less inductive path

    Lightning currents flow radially from the point of injection

    (earth electrodes) embedded in the earth

    Providing multiple paths for current injection into theinterface; reducing overvoltages

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    IEC 62305 10 d d

    Proposed TIA B

    Grounding System Performance

    Criteria Resistance-to-earth

    2ndNFPA 7025 or drive electrode

    DoD / DOE Explosives

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    Circuit Model

    Z =R +jLG +jC

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    Impedance vs. Resistance

    Resistance

    often dominated by earth resistivity

    increases with frequency due to skin effect

    Inductance

    influenced by geometry of conductors / electrodes

    increased by bends in conductor routing

    Capacitance

    dominated by electrode-to-earth interface

    v(t) = i(t) R + L (di/dt) + i(t) / C = i(t) Z

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    Impedance Measurement Method

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    300 m

    Vertical Rod in 300 m soil

    FREQUENCY IN Hz

    vertical rod

    300 .m

    IMPEDANCE in

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    d i t it

    120 )

    Vertical Rod in 300 m soil

    Impedance decreases with frequency due todominate capacitance

    Impedance high even in low resistivity soil (70 to

    120 ). Additional experiments (data not shown)

    Same behaviour found for horizontal grid in 300 msoil

    3 rods in triangle in 200 .m soil : Z constant (3040 )

    Earth Enhancement Compound decreases localresistivity and improves contact (decreases R and Z)

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    c row foot

    Crow Foot Arrangement in

    Rocky SoilIM P E D AN C E in

    F R E Q UE NC Y IN Hz

    cro w footro ck y so il

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    Effi i t li ht i t ti di

    Crow Foot Arrangement in

    Rocky Soil 200 m soil Low increase of impedance (Z)

    Less than 20 ohms change across entirefrequency spectrum

    Efficient lightning protection grounding

    system

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    110 m

    25 meter long Horizontal Tape

    FREQUENCY IN Hz

    25 m horizontal tape

    110 .m

    IMPEDANCE in

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    25 meter long Horizontal Tape

    Low increase of impedance (Z)

    20 ohms change from 10 Hz to 1 MHz

    50 m deep well

    Z = 10 at low frequency / 70 at 1MHz

    Additional experiments (data not shown)

    Z almost doubles for 50 meters of tape

    Similar behavior from 20 m to 50 m verticalwell in 200 m soil

    Buried 0.5 meters in 110 m soil

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    Driven rod for cabinet

    Telecom Application

    3 legged tower

    Equipment cabinet

    Driven rod per leg

    Driven rod for cabinet

    Ground loop

    conductor tyingtogether driven rods

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    Tower Leg Impedances

    South Tower Leg East Tower Leg

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    Tower Test Points

    South Tower Leg East Tower Leg

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    Cabinet Ground Impedance

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    (1MH ) C bi t 79 2 t 52

    SummaryofObservations

    test badgiven HF criteria

    Data from tower legs similar (w/in 3 )Effect of ground rods noted @ 202 kHz

    R (tower legcabinet bus) = 1 m

    Bend in solid wire between copper bus bar

    and grounding electrode shows up as L

    Rgnd Cabinet = South tower leg = 9

    Rgnd (1MHz): Cabinet =79.2; tower = 52

    All 3 less than 10 @ low frequency but

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    Impedance Accep tance Cri ter ia

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    CaseStudies

    E: Group of Chimneys

    F: Metallic Tanks

    A: Building with large grounding system

    B: Factory Extension

    C: Metal Silos D: Metallic-framed Shed

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    ES 1002

    Mesure 14

    Nombre de points 20

    80

    100 1000 10000 100000 1000000

    -60

    ZR

    X(OH

    M)

    60

    40

    20

    0

    -20

    Z

    R

    X

    -40

    Frquence (Hz)

    Case A: Building with large earthing system

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    Case B: FactoryExtension

    Extension of existing

    Clearly a bad earthing

    factory

    Bad soil, mainly rocks Crow foot system

    R = 150

    system

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    Case B: Building with a crow foot in bad soil

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    Case C: Metallic Silos

    Small contact surface between metal and soil

    R = 15

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    50

    30

    -20

    ohms

    130

    120

    110

    100

    90

    80

    70

    60 Z

    40 R

    20

    10

    0

    -10 X

    -30

    -40

    10 100 1000 10000 100000 1000000Fre que ncy (Hz)

    Case C: Silo in contact with soil

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    Case D: Large shed with metallic frame

    R = 4

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    30

    50

    30

    -30

    Z

    R

    ohms

    130120

    110

    100

    90

    80

    70

    60

    40

    2010

    0

    -10

    -20 X

    -40

    -50

    10 100 1000 10000 100000 1000000

    Frequency (Hz)

    Case D: Shed with metallic frame

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    thi t

    Case E: Group of Chimneys

    Earthing on each chimney

    Connected togetherby copper tape

    R = 5

    Good low frequency

    resistance but gets

    very high at frequencies

    above 100 kHz bad lightning

    earthing system

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    50

    30

    -30

    Frequency (Hz)

    R

    X

    ohms

    130

    120110

    10090

    80

    70

    60 Z40

    20

    10

    0-10

    -20

    -40

    -50

    -60

    -70

    -80

    10 100 1000 10000 100000 1000000

    Case E: Group of chimneys

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    Case F: Metallic Tanks

    Tank diameter 6 meters

    Near the sea

    Concrete baseimmersed in

    sand/watermixture

    No dedicated

    earthing system

    R = 1

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    50

    30

    -30

    10 100 1000 10000 100000 1000000

    R

    X

    ohms

    130120

    110

    100

    90

    80

    70

    60 Z40

    20

    10

    0

    -10

    -20

    -40

    -50

    -60

    -70

    -80

    Frequency (Hz)

    Case F: Metallic tank near the sea

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    E l f id ti

    Proposed Criteria Development

    earthing system to dissipate lightning current while

    minimizing overvoltages

    Examples for consideration:30 from low frequency to 1 MHz10 at low frequency and 100 at high frequencies ?

    To evaluate the earthing systems we will calculate

    the voltage generated by the injection of a 10 kA1/20 current pulse into the earthing impedance

    measurements reported earlier.

    Determine equivalent resistance (RHF)

    Difficult to establish a single criteria for quality of

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    ( 46 40 4

    SummaryofResults

    The mean value of the measured impedance between 63 kHz and 1 MHz

    (Mean Z) computed from data provided by high frequency earth impedancetest equipment.

    This value is consistent with RHF and is suggested as criterion

    Z Impedance value ()

    Case A Case B Case C Case D Case E Case F

    RLF () 4 150 15 4 5 1RHF () 47 203 35 22 47 16

    Mean Z () 46.7 184 40.7 22.9 45.5 17.9

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    ProposedCriteria

    10