roadmap for assessment of lightning mitigation technologies

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    Non-Conventional

    Lightning Mitigation:

    Fact or Fiction?

    IEEE PES

    2003 General Meeting

    July 16, 2003

    A Roadmap for

    Evaluation of

    Lightning EliminationTechnologies

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    Purpose of Talk

    Review methods that have been used to observeperformance:

    Small or large-scale high-voltage tests usingelectrostatic or switching-impulse excitation

    Anecdotes and Lack of Damage

    Visual Inspection for Damage

    Visual Observations during Storms

    Measurements of DC or impulse current

    Remote measurements from lightning location

    systems

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    Introduction

    Lightning control or mitigation has beenproposed with a wide range of treatments:

    The Franklin Rod, a conductive electrode

    that provides a preferred path for lightning.

    Multiple shells of conductive material,providing increased protection to the interior

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    Conventional Protection IEC 61312

    Dehn & Shne, 1995

    Zone 1

    Zone 0

    Zone 2

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    Introduction

    Lightning control or mitigation has beenproposed with a wide range of treatments:

    Small conductive electrodes that modify theelectric field, making them more attractive tolightning than a conventional lightning rod.

    -Concept of critical radius in switching surge testing

    - Rocket triggered lightning

    Largeconductive electrodes that modify theelectric field to make a structure less attractiveto lightning.

    - Rod-plane versus sphere-plane gap flashover

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    Introduction

    Lightning control or mitigation has beenproposed with a wide range of treatments:

    Semiconductive electrodes intended to limitpeak current and rate of current rise.

    Semiconductive electrode extensions such

    as laser plasma, liquid jets, glow discharge orstreamers, ionizing radiation

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    Laboratory Studies

    High-voltage facilities and resources for adequatestudy of leader development are not widely

    available.Unfortunately, extrapolation of reduced-scalecorona and nonlinear field effects from small to

    larger physical scales has usually beenproblematic.

    streamer formation process dominates the impulse

    flashover of 0.1-m gaps flashover of 1-m gaps is dominated by leaderformation, with streamer formation contributing a

    minor time delay.

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    Laboratory Studies Small Scale

    200 kV/m

    570 kV/m

    300 kV/m

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    Typical Laboratory Study - Grounding

    800 kV, 2us impulse, http://www.deutsches-museum.de/ausstell/dauer/starkst/e_strom2.htm#top

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    Typical Field Observations

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    Laboratory Studies

    Physics of switching-surge flashover at 3-15 m scale hasbeen extrapolatedto the final jump of the lightning,a process that occurs over a 30 to 200-m gap.

    Positive switching-surge leaders have speeds of 104 m/s,currents of 0.4A, and linear charge of about 40C/m.Corresponding values for natural lighting are 105 m/s,100A and 1000C/m.Even so, the resulting models [Rizk, Dellera-Garbagnatiadapted by Tarchini] describe many of the same features

    as the Electrogeometric model (EGM) that relates theobserved reach of the final jump to the current in theresulting flash.

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    Laboratory Studies

    Laboratory tests of spherical tips or enhanced airterminals in large rod-to-plane gaps have been usedto address questions of theoptimal size and shapeoftreatments, whether intended to increase or decreasestroke incidence.

    Comparison tests of treated and untreated rods are

    sensitive to height: An advantage of less than 0.03mwas noted in tests comparing a 72-Curie radioactivesource treatment to a rod.

    There is increased leader inception and switching-surge flashover voltage in a 7-m gap for a criticalelectroderadius of greater than 0.4m.

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    Typical Field Observations

    Lightning triggered by

    airplane- Upward branching to sky- Downward branching to

    ground- Commercial airplanestypically struck once a year

    - Most flashes triggered bythe presence of the airplane

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    Electric Field Mapping

    LAUNCH PAD LIGHTNINGWARNING SYSTEM (LPLWS)

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    Electric Field Mapping

    LAUNCH PAD LIGHTNINGWARNING SYSTEM (LPLWS)

    Total of 36 flashesin 100 km2

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    Anecdotal Interpretation

    There was lightning all around.

    The flash-to-bang time was less than 15 seconds.

    My 220-m (720) tower, recently treated, was notstruck.

    The treatment works.

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    -7.3 kV/m

    Models for Flash Incidence to Towers

    96.0248.0

    600211.0)9.25(

    10hNh

    NN g

    g

    d

    Downward Flashes

    hkVEgc 1600

    Upward Flashes

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    Quantitative Interpretation

    There was a storm flash density of 0.36/km2.

    The expected number of downward flashes to a220-m tower on flat ground would be0.13, basedon the storm flash density.

    The expected number of upward flashes from a220-m tower on flat ground would be0.033,based on the observed ground-level field

    strength values.

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    Quantitative Interpretation

    To see a conclusive (2-) difference in treatment, onewould need to observe for a period that would haveproduced n flashes, where

    This means that:

    4/0.13 = 31 similar storms need to be observed to

    comment on the treatment for downward flashes.121 storms would need analysis for upward flashesbased on this distribution of ground-level electric fields.

    4

    220

    n

    nnn

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    Quantitative Interpretation

    Year-to-year variations in storm exposure canbe large: Ng at Bruce NGS

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    Example of Adequate Comparison Study

    N. Kuwabara, T. Tominaga, M. Kanazawa, and S. Kuramoto, Probability Occurrenceof Estimated Lightning Surge Current at Lightning Rod before and after InstallingDissipation Array System (DAS),1999 IEEE Intl EMC SymposiumPaper 00476,Seattle WA, ISBN 0-7803-5638-1

    Before Treatment:26 surges recorded in three years.

    After Treatment*:

    16 surges recorded in one year.

    After Correction for Storm Exposure:

    No difference, treated / untreated.* The treatment was penetrated by a 2-m lightning rod, which wouldhave been enveloped by any corona envelope greater than 2 m.

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    Example of Adequate Comparison Study

    N. K uwabara, T. Tominaga, M. Kanazawa, and S. Kuramoto, Probability Occurrence ofEstimated Lightning Surge Current at Lightning Rod before and after Installing Dissipation ArraySystem (DAS), 1999 IEEE Intl EMC SymposiumPaper 00476, Seattle WA, ISBN 0-7803-5638-1

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    Lightning Location Systems

    In continental USA/Canada, a sophisticatedand accurate network of receivers has

    provided lightning location and amplitudedata since the mid 1990s.

    The technology is based on GPS time ofarrival and direction finding based on the

    strong radiation from a vertical lightningchannel.

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    199906111330.000000

    30 kA

    Lightning Location Technology

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    199906111330.000420

    199906111330.0004216 118.6 45.0

    Lightning Location Technology

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    199906111330.000960

    199906111330.0004216 118.6 45.0

    199906111330.0009613 52.0 135.0

    Lightning Location Technology

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    199906111330.001080

    199906111330.0004216 118.6 45.0

    199906111330.0009613 52.0 135.0

    199906111330.0010536 47.4 270.0

    Lightning Location Technology

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    199906111330.0004216 118.6 45.0

    199906111330.0009613 52.0 135.0

    199906111330.0010536 47.4 270.0

    T=92.3 s

    T=539.7 s T=632.0 s

    Lightning Location Technology

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    199906111330.0009613 52.0 135.0

    Lightning Location Technology

    199906111330.0010536 47.4 270.0

    199906111330.0004216 118.6 45.0

    DD+28 km

    Hyperbola withT=92 s (28 km)

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    Lightning Location System Performance

    Location accuracy ofmeasured data from

    ALDIS (GAI) lightningdetection network forcorrelated strokes to a

    100-m tower inGaisburg, Austria.

    The tower is centeredat the origin.

    G. Diendorfer, W. Hadrian, F. Hofbauer, M. Mair, W. Schultz, Evaluation of Lightning Location Data Employing

    Measurements of Direct Strikes to a Radio Tower, CIGRE Session 2002, paper 33-206

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    LLS Observation of Treated Area

    FEDEX installation in Memphis, TN

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    LLS Observation of Treated Area

    FEDEX installation in Memphis, TN

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    LLS Observation of Treated Area

    FEDEX installation in Memphis, TN

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    LLS Observation of Treated Area

    FEDEX installation in Memphis, TN

    Correct Size of Dots,

    Based on 400-m Uncertainty

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    Conclusions

    Anecdotal data: There was lightning allaround but the treatment was not struck is

    inconclusive for typical structure heights andtypical reporting periods.

    Quantitative data: The ground-level electricfield Ez >(1600/h) , the treatment reacted and

    was/was not struck, instead a nearbystructure/ground was struck.

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    Conclusions

    Transfer functions are needed between:

    Excitation (local static or dynamic

    vertical electric fields) and

    Treatment effects (visible, UV corona or

    related currents)

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    Conclusions

    Lightning location system data are essential:

    For validating time-tagged records of structure

    currentsFor normalizing observations of performance

    However, holes in the data before and aftertreatment need to be larger than 400-mobservation error and should have enough samplesto be convincing. Locally,

    While globally, nafter= nbefore

    beforebeforeafterafter nnnn 22

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    Conclusions

    Direct rather than indirect measurements areneeded to assess treatments.

    Before and after treatment, with a minimumof four responses in one group and noresponses, for the same lightning exposure, in

    the other group, is convincing.Damage to equipment is a poorly-calibratedmeasure of response, since replacement

    equipment often has different (and higher)surge absorption capability.