1 Earth Testing 2010

Embed Size (px)

Citation preview

  • 7/27/2019 1 Earth Testing 2010

    1/68

    1

    Earth Testing

  • 7/27/2019 1 Earth Testing 2010

    2/68

    2

    Earth Testing Pioneer

    Dr George Tagg pioneered earth testing at Megger

    Designing, manufacturing and selling for well over

    50 years

  • 7/27/2019 1 Earth Testing 2010

    3/68

    3

    Earthing System ResistancePurpose : Measure resistance of earthing system to Earth - ascertain thatprospective fault current can be conducted safely to Earth and thus limittouch voltage.

    Methods : 3-pole: Fall of Potential 2-pole: Direct measurement

    3-pole:Slope Method 3-pole with clamp Stakeless measurements: Earth Clamp.

    Note:

    The earth electrode under test must be disconnected from the system itis earthing (apart from clamp & stakeless measurements)

  • 7/27/2019 1 Earth Testing 2010

    4/68

    4

    Step and touch voltages

    V V

    Step Touch

  • 7/27/2019 1 Earth Testing 2010

    5/68

    5

    Resistance and GPR from earth electrode

    0.0

    0.4

    0.8

    1.2

    1.6

    2.0

    R e s i s t a n c e ( O h m s )

    0

    200

    400

    600

    800

    1000

    V o l t a g e ( V )

    Resistance GPR

  • 7/27/2019 1 Earth Testing 2010

    6/68

    6

    Earth sphere of influence

    Resistance of an earth electrode 1 Resistance of the electrode and the

    connections to it (low)

    2 Contact resistance of the surroundingsoil to the electrode (should be low)

    3 Resistance of the surrounding body ofearth around the electrode these can be

    thought of as shells and create a sphere ofinfluence (varies)

  • 7/27/2019 1 Earth Testing 2010

    7/68

    7

    2-pole: Direct measurementMeasure coupling between two earth points; measureresistance of earth electrode to Earth .

    C1 (E)C2 (H)P1 (ES)P2 (S)Imeas

    Emeas

    Earth electrodeunder test

    Second earth electrode or other

    low resistance, conductiveconnection to Earth.

    Measures resistance ofthe two Earth electrodesin series.

    R = E meas /Imeas

  • 7/27/2019 1 Earth Testing 2010

    8/68

    8

    2-pole Method Advantages

    Quick and easy

    Better than a continuity measurement with amultimeter because of noise rejection

  • 7/27/2019 1 Earth Testing 2010

    9/68

    9

    2-pole Method Disadvantages

    Result is a loop resistance, not just the electrode wewant to measure but the return path as well

    Only OK if we have a good known low value returnpath and a high resistance electrode under testInterfering spheres of influence can give incorrect

    results

  • 7/27/2019 1 Earth Testing 2010

    10/68

    10

    3-pole: Fall of Potential (full method)Classic method for measuring resistance of a singleearthing electrode, or of a system of electrodes to

    Earth.

    A

    B

    C1 (E)

    C2 (H)P1 (ES) P2 (S)

    Imeas

    Emeas

    Earth

    electrodeunder test

    Auxiliary test

    electrodes

    R = E meas /Imeas

  • 7/27/2019 1 Earth Testing 2010

    11/68

    11

    Fall of Potential - Full MethodVary location of P2 (Potential) spike by regular steps

    along a straight line between the electrode under test and

    the C2 (Current) electrode.

    Take resistance R = E meas /Imeas at each step and plot agraph of R versus distance.

    Resistance of system taken where slope is flat.

    NB The C spike must be outside the sphere of influence

    to achieve a viable reading

  • 7/27/2019 1 Earth Testing 2010

    12/68

    12

    Fall of Potential Method Advantages

    Can always make an accurate measurement of earthresistance

    Measures the overall system resistance at this point,to calculate earth fault currentTest leads & contact resistance are not included in

    the measurement (may want to use 4 terminals)Can check by testing in a different direction ordistance

  • 7/27/2019 1 Earth Testing 2010

    13/68

    13

    Fall of Potential Method Disadvantages

    Extremely time consuming and labour intensive.- Temporary probes must be placed.

    - Cables must be run to make connections.Space constraints can make it hard to place remoteprobes.Must disconnect individual ground electrodes tomeasure them.

  • 7/27/2019 1 Earth Testing 2010

    14/68

    14

    Fall of potential - Current Probe Sphere of Influence

    AuxiliaryCurrent

    Probe (C)

    AuxiliaryPotentialProbe (P)

    GroundElectrode

    UnderTest (X)

    P probe must be outside of both

    spheres of influence for correctmeasurement

  • 7/27/2019 1 Earth Testing 2010

    15/68

    15

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    16/68

    16

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    17/68

    17

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    18/68

    18

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    19/68

    19

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    20/68

    20

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    21/68

    21

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    22/68

    22

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    23/68

    23

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    24/68

    24

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    25/68

    25

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Positions

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    26/68

    26

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Position

    GroundElectrodeUnder

    Test (X)

    True systemresistancemeasuredhere

  • 7/27/2019 1 Earth Testing 2010

    27/68

    27

    Fall of potential test and result

    CurrentProbe

    Position

    Distance of Potential Probe from X (d p)Ground

    ElectrodePosition

    X C

    R e s

    i s t a n c e

    i n O h m s

    CurrentProbe (C)

    PotentialProbe (P)Position

    GroundElectrodeUnder

    Test (X)

    True systemresistancemeasuredhere

    Usually approx 62%of X to C distance

  • 7/27/2019 1 Earth Testing 2010

    28/68

    28

    For deeper spikes -Readings are taken further apart

    Guidelines for setting test probes are based on the depth of the electrode under test.

    2m depth p spike 15.5m c spike 25m

    3m depth p spike 18.5m c spike 30m

    6m depth p spike 25m c spike 40m

    10m depth p spike 31m c spike 50m

  • 7/27/2019 1 Earth Testing 2010

    29/68

    29

    3-pole: Fall of Potential (short method)

    Site P2 (Potential) spike at 62% of B and take resistancemeasurement R a[R = E meas /Imeas ].

    Locate P2 0.1B around the 62% point and take additionalresistance readings, R b and R c .

    If the three readings are within an agreed accuracy limit, thesystem resistance is the average.

  • 7/27/2019 1 Earth Testing 2010

    30/68

    30

    The Problem of Limited Distance/Space

    Distance of Potential Probe from X (d p)

    R e s i s t a n c e

    i n O h m s

    CurrentProbe (C)PotentialProbe (P)

    GroundElectrodeUnder

    Test (X)

  • 7/27/2019 1 Earth Testing 2010

    31/68

    31

    The Slope Method

    Based on the theory behind the Fall of Potential method:- for complex grounding systems and/or- situations where lead lengths prohibitive

    This method allows measurement of the earth systemresistance without finding the flat portion of the curve,reducing the test distances

    Use three measurements in calculation; can take more

    Advantage: Provides an approach for dealing with complexsystems

    Disadvantage: Less accurate; requires more maths

  • 7/27/2019 1 Earth Testing 2010

    32/68

    32

    3-pole: Slope Method

    Tables of values for the co-efficient of slopeagainst actual P spike distance is published in the

    instrument user guide

    Take calculated value of and look up idealdistance of the voltage spike (P2) for measuring theelectrode resistance

  • 7/27/2019 1 Earth Testing 2010

    33/68

    33

    3-pole: Slope Method

    Vary location of P2 (Potential) spike by regularsteps along a straight line between the electrode

    under test and the C2 (Current) electrodeMeasure resistance at each step and plot a graph

    of R versus distance.Measure resistance at 0.2B, 0.4B and 0.6B: R1,

    R2 and R3.Slope coefficient, =(R3-R2)/(R2-R1) relatesdistance B and ideal distance of the voltage spike

    (P2) for measuring the resistance.

  • 7/27/2019 1 Earth Testing 2010

    34/68

  • 7/27/2019 1 Earth Testing 2010

    35/68

    35

    3-pole: Slope Method

    Measure R1 at 20% distance to C2

    C2 (H)

    Earthelectrode

    under test

    B

    C1 (E)

    P1 (ES)

    Imeas

    Emeas

    0.2B

    R1

    C2 (H)

    =(R 3-R2)/(R2-R1)

    = (R 3-R2) / (R 2 9.3 )

    R1= 9.3 ohm

    R = E meas /Imeas

  • 7/27/2019 1 Earth Testing 2010

    36/68

    36

    3-pole: Slope Method

    Measure R2 at 40% distance to C2

    C2 (H)

    Earthelectrode

    under test

    B

    C1 (E)

    P1 (ES)

    Imeas

    Emeas

    0.4BR2

    C2 (H)

    =(R 3-R2)/(R2-R1)

    = (R 3 16 ) / (16 9.3 )

    R1= 9.3 ohmR

    2= 16 ohm

    R = E meas /Imeas

  • 7/27/2019 1 Earth Testing 2010

    37/68

    37

    3-pole: Slope Method

    Measure R3 at 60% distance to C2

    C2 (H)

    Earthelectrode

    under test

    B

    C1 (E)

    P1 (ES)

    Imeas

    Emeas

    R30.6B

    C2 (H)

    =(R3-R2)/(R2-R1)

    = (19.2 16 ) / (16 9.3 )

    R1= 9.3 ohmR

    2= 16 ohm

    R3= 19.2 ohm

    R = E meas /Imeas

  • 7/27/2019 1 Earth Testing 2010

    38/68

    38

    3-pole: Slope Method

    Calculate value of

    C2 (H)

    Earthelectrode

    under testB

    C1 (E)

    P1 (ES)

    P2 (S)

    Imeas

    Emeas

    0.4B

    0.6B

    0.2B

    Auxiliary testelectrodesR3R2R1

    C2 (H)C2 (H)

    =(R 3-R2)/(R2-R1)

    = (19.2 16) / (16 9.3)

    =0.478

    R = E meas /Imeas

  • 7/27/2019 1 Earth Testing 2010

    39/68

    39

    3-pole: Slope Method

    =0.478

  • 7/27/2019 1 Earth Testing 2010

    40/68

    40

    The Slope Method

    R1 = 0.2 x D C; R 2 = 0.4 x D C; R 3 = 0.6 x D CCalculate the value for using the following equation:

    R3 - R2R2 - R1

    The value for corresponds to a value for P T /C.- PT: potential probe position where True Resistance found.- % of distance P T is of D C.- Table of values in Getting Down to EarthMeasure the resistance at P T.Repeat the process for a larger value of C.

    Factors Affecting Resistance Variation

  • 7/27/2019 1 Earth Testing 2010

    41/68

    41

    Type of ground composition beneath the site

    Moisture content of soil (tides, rainfall, season)

    Quantity and type of electrolytes added to the soil

    Adjacent conductors if any

    Temperature of the earth

    Electrode depth

    Electrode diameter

    Electrode(s) spacing

    See 62% rule

    Twice diameter = -20%

    - 40% (x2 indepth)

    + 20% for - 10 o(ICE is very high)

    ?

    < 10 x lower

    60%

    Large 10/1

  • 7/27/2019 1 Earth Testing 2010

    42/68

    42

    Soil Resistivity/ Wenner Method

    Purpose: Survey a site for the lowest resistanceconnections for Earth.

    A A A

  • 7/27/2019 1 Earth Testing 2010

    43/68

    43

    Purpose of this test: Find lowest possible resistance in a location Obtain the values needed to design the earth system

    Factors affecting soil resistivity Soil composition Moisture in the ground Temperature

    Consider Resistivity will vary through the year Moisture more constant at water table

    Stable temperature below the frost line

  • 7/27/2019 1 Earth Testing 2010

    44/68

    44

    Soil Resistivity typical values (Ohm-cm)

    Surface soils, loam etc. 100 5000Clay 200 10000

    Sand & gravel 5000 100000Surface limestone 10000 1000000Shales 500 10000

    Sandstone 2000 200000Granites, basalts etc 100000Slates etc 1000 10000

    What Can Be Done to Improve Earth Resistance?

  • 7/27/2019 1 Earth Testing 2010

    45/68

    45

    What Can Be Done to Improve Earth Resistance?

    Lengthen earth electrode

    Increase the rods diameter

    Use multiple electrodes bonded together

    Treat the surrounding soil chemically

  • 7/27/2019 1 Earth Testing 2010

    46/68

    46

    Application of ART

    Potential Probe (P) CurrentProbe (C)

    GroundElectrodes

    Building earthconnection/s

    I Total

    I System

    Ie1

    Ie 2Ie 3Ie test Test

    Ie Test > I Total20

    XConnection

    l k l h d l

  • 7/27/2019 1 Earth Testing 2010

    47/68

    47

    Clamp-On / Stakeless Methodology

    GroundElectrode

    UnderTest

    Building earthconnection/s

    ICLAMP

    VCLAMP

  • 7/27/2019 1 Earth Testing 2010

    48/68

    48

    Stakeless Measurements for earthsystem resistance (DET10/20C)

    A method that does not needthe earth electrode to bedisconnected

    R =Emeas /Imeas

    Rx

    R1

    R2

    Rn

    EmeasImeas

  • 7/27/2019 1 Earth Testing 2010

    49/68

    49

    Clamp-On Method

    Includes the bonding and overall connectionresistance (not available with Fall of Potential).

    Can measure the leakage current flowing throughthe system.Effective only in situations with multiple grounds inparallel (pole grounds).Cannot be used on isolated grounds (no returnpath)Cannot be used if an alternative lower resistance

    return exists not involving the soil

  • 7/27/2019 1 Earth Testing 2010

    50/68

    50

    Clamp-On/Stakeless Methodology

    In a multiple ground system the circuit can beconsidered a loop comprising:- The individual ground electrode.

    - A return path via all other electrodes.- The mass of earth.

    The single electrode will have a higher resistancethan the remainder of grounds connected in parallel.

    Inject a voltage and measure the resultant currentproduced in a single turn ground loop.

    Clamp On/Stakeless Methodology

  • 7/27/2019 1 Earth Testing 2010

    51/68

    51

    R 6R 5R 4R 3R 2R 1

    VI

    Clamp-OnGroundTester

    Clamp-On/Stakeless Methodology

    R loop = V loop / I loop

    Cl O /S k l M h d l

  • 7/27/2019 1 Earth Testing 2010

    52/68

    52

    Clamp-On/Stakeless Methodology

    R loop = R 6 + (1/(1/R 1 + 1/R 2 + 1/R 3 + 1/R 4 + 1/R 5))For 6 similar electrodes with a resistance of 10 :R loop = 10 + 2 = 12

    If one electrode has a resistance of 100 :R loop = 100 + 2 = 102 (measuring the bad electrode)R loop = 10 + 2.4 = 12.4 (on the other electrodes)

    For 60 similar electrodes with a resistance of 10 :R loop = 10 + 0.17 = 10.17

    If one electrode has a resistance of 100 :R

    loop= 100 + 0.17 = 100.2 (measuring the bad electrode)

    R loop = 10 + 0.17 = 10.17 (on the other electrodes)

    Cl O M h d Ad

  • 7/27/2019 1 Earth Testing 2010

    53/68

    53

    Clamp-On Method - Advantages

    Test is quick and easy:- No disconnecting the ground rod from the system.- No probes need to be driven/cables connected.

    Includes the bonding and overall connection resistance(not available with Fall of Potential).Can measure the leakage current flowing through the

    system..

  • 7/27/2019 1 Earth Testing 2010

    54/68

    54

    Clamp-On Method - Disadvantages

    Effective only in situations with multiple grounds in parallel (polegrounds).Cannot be used on isolated grounds (no return path):- Not applicable for installation checks/commissioning new sitesCannot be used if an alternate lower resistance return exists notinvolving the soil:- Cellular towers- Substations

    Subject to influence if another part of the ground system is inresistance area:- Result will be lower than true resistance.Test is carried out at a high frequency (enables the transformers

    to be small):

    - Less representative of a fault at power frequency but easier to filter outnoise

    Cl O M h d Di d

  • 7/27/2019 1 Earth Testing 2010

    55/68

    55

    Requires a good return path:- Poor return path may give high readings.

    Connection must be on the correct part of the loop for

    the electrode under test:- Requires thorough understanding of the system.- Wrong connection can give a faulty result.

    Susceptible to noise from nearby substations and

    transformers (no reading).No basis for the test in standards no objective

    reference for the test resultsLess effective for very low grounds:

    - Extraneous elements in reading become comparatively large.

    Clamp-On Method - Disadvantages

    Cl O M h d R d i

  • 7/27/2019 1 Earth Testing 2010

    56/68

    56

    Should not use as the only test instrument unless theearth system architecture is known and understood

    Is an important part of the ground testing tool kit.- Should also have a Fall of Potential tester.

    Use the Clamp-On to identify potential problems

    quickly; confirm with a Fall of Potential tester:- Saves time.- Ensures accuracy- No disturbance of connections or re-connection risks

    Clamp-On Method - Recommendations

    A li i l G d

  • 7/27/2019 1 Earth Testing 2010

    57/68

    57

    Grounding

    Conductor

    GroundRod

    ButtPlate

    UtilityPole

    Applications Pole Grounds

    A li i S i E /M

  • 7/27/2019 1 Earth Testing 2010

    58/68

    58

    Applications Service Entrance/Meter

    GroundRods

    ServiceBox

    ServiceMeter

    Pole-MountedTransformer

    A li ti S i E t /M t

  • 7/27/2019 1 Earth Testing 2010

    59/68

    59

    Applications Service Entrance/Meter

    WaterPipe

    ServiceBox

    ServiceMeter

    Pole-MountedTransformer

  • 7/27/2019 1 Earth Testing 2010

    60/68

    Applications Pad Mount Transformer

  • 7/27/2019 1 Earth Testing 2010

    61/68

    61

    Applications Pad Mount Transformer

    EnclosureOpen

    Door

    Open

    Door

    Underground Service

    ConcentricNeutral

    Buss

    GroundRod(s)

    Service

  • 7/27/2019 1 Earth Testing 2010

    62/68

    Applications Transmission Towers

  • 7/27/2019 1 Earth Testing 2010

    63/68

    63

    Applications Transmission Towers

    Ground

    Rod

    Applications Telephone Cabinets

  • 7/27/2019 1 Earth Testing 2010

    64/68

    64

    pp p

    GroundRod

    TelephoneCable orConduit

    GroundWire

    AC Panel Board

    Power MeterL-N/L-L Vac

    Power Service

    BondingIntegrity

    GroundResistance

    Misuses Cellular Sites

  • 7/27/2019 1 Earth Testing 2010

    65/68

    65

    Clamp-OnGroundTester

    TestCurrent

    Misuses Cellular Sites

    Misuses Substations

  • 7/27/2019 1 Earth Testing 2010

    66/68

    66

    SubstationGroundedPerimeter

    Fence

    E

    Clamp-OnGroundTester

    SubstationGroundSystem

    TestCurrent

  • 7/27/2019 1 Earth Testing 2010

    67/68

    67

    ERR

    OR

    OFFEN

    STA

    CK

  • 7/27/2019 1 Earth Testing 2010

    68/68

    :

    u

    n d e

    f i n

    e d

    DIN

    G C O

    MMAND

    : f ~

    :