Recent Research ch on Lightning, with Implications f s for Air - - PowerPoint PPT Presentation

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Recent Research ch on Lightning, with Implications f s for Air - - PowerPoint PPT Presentation

Recent Research ch on Lightning, with Implications f s for Air Terminals William William am Rison am Rison Professor of Elect ectrical Engineering New Mexico Institute of of Mining and Technology Socorro, Ne , New Mexico Recent


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SLIDE 1

Recent Research with Implications f

William William

Professor of Elect New Mexico Institute of Socorro, Ne

ch on Lightning, s for Air Terminals

am Rison am Rison

ectrical Engineering

  • f Mining and Technology

, New Mexico

slide-2
SLIDE 2

Recent Lightning Implications for

Computer Modeling of t

Process

High Speed Videos of th

Process Process

ing Research with for Air Terminals

f the Lightning Attachment f the Lightning Attachment

slide-3
SLIDE 3

Video by Tom Warner, June 17, 2007, ne

High Speed Negative Cloud to G 7,100 Frames

17, 2007, near Devil’s Tower, Wyoming

eed Video of to Ground Discharge es per Second

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SLIDE 4

Video by Tom Warner, June 17, 2007, ne 17, 2007, near Devil’s Tower, Wyoming

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SLIDE 5

Video by Tom Warner, August 4, 2007, ne

High Speed Attachment P Negative Cloud to G 7,100 Frames

500 foot tall tower 4, 2007, near Rapid City, South Dakota

eed Video of t Process for a to Ground Discharge es per Second

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SLIDE 6

History of Attempt for ESE Air

1980’s --- Laboratory ex

100 µs time advantage fo

Early 1990’s --- Push by

adoption of an ESE stand adoption of an ESE stand

1990’s --- Prolonged pro

  • ver proposed NFPA sta

Early 2000’s --- NFPA d

standard and retain NFP

2005 through 2008 --- Fe

ESE manufacturers

pt to Pass a Standard ir Terminals

experiments indicate e for ESE air terminals by ESE manufacturers for andard andard procedural and legal fight standard decides to reject ESE FPA 780 Federal court rules against

slide-7
SLIDE 7

History of Attempt for ESE Air

ESE based on three assu

1)

Laboratory time advant present in real lightning

2)

Initial early streamer w

2)

Initial early streamer w upward leader

3)

Upward leader speed is

If these three assumption

ESE terminals a 100 met

No input from scientific

development of standard

pt to Pass Standard ir Terminals

sumptions

antage of about 100 µs will also ing will develop into successful will develop into successful is about 1 x 106 m/s

ions are true, they will give eter capture radius fic community on ard

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SLIDE 8

History of Attempt for ESE Air

No scientific consensus

when the standard was p

pt to Pass Standard ir Terminals

us on ESE assumptions at s proposed

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SLIDE 9

Validity of ESE

1)

Laboratory time advantage of 100

  • No scientific research indica
  • Golde (1941), “The Validity

Models”

  • “there is a question regar

test designed to simulate leader and the attachment lengths, tens of meters, e experiment” (Rakov & U

  • Becerra and Cooray (2008),

be Utilized to Justify the Act Terminals”

SE Assumptions

100 µs also present in real lightning ndicating that this is the case dity of Lightning Tests with Scale garding the validity of any laboratory te the physics of the lightning stepped ent process, since typical leader step , exceed the size of the laboratory Uman, 2003) 2008), “Laboratory Experiments Cannot ction of Early Streamer Emission

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SLIDE 10

Validity of ESE

2) Initial early streamer w

successful upward lead

  • No research at time sta
  • Moore et al (2000) “Me
  • Moore et al (2000) “Me

Rod Responses to Near streamers ineffective

SE Assumptions

r will develop into ader

standard proposed Measurements of Lightning Measurements of Lightning earby Strikes” shows early

slide-11
SLIDE 11

Validity of ESE SE Assumptions

Early streamers do not develop into leaders

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SLIDE 12

Validity of ESE

3) Upward leader speed is

  • Not many measuremen

time standard proposed

  • Now, several measurem
  • Now, several measurem

speed of about 1 x 105

  • Tom Warner tower stri

1.2 x 105 m/s

  • Speed of 1 x 105 m/s gi

radius

SE Assumptions

d is about 1 x 106 m/s

ents of upward leader speeds at sed rements of upward leaders show rements of upward leaders show m/s trike video: average speed of gives only 10 meter capture

slide-13
SLIDE 13

Validity of ESE

  • Research since the ESE

shows all three ESE as

  • There have been no ind

showing ESE terminals showing ESE terminals

  • There is now scientific

terminals are ineffectiv

  • It was premature to ado

terminals in early 1990

SE Assumptions

SE standard was proposed assumptions are incorrect independent field studies als are effective als are effective fic consensus that ESE tive adopt a standard for ESE 90’s

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SLIDE 14

CVM H

  • Idea initially proposed by
  • Theory was further develo

Gumley(2000) and D’Ales

  • Tested by D’Alessandro in

Kong (Petrov & D’Alessan Kong (Petrov & D’Alessan and Petrov, 2006)

History

y Eriksson (1979) eloped by D’Alessandro and lessandro (2002) in Kuala Lumpur and Hong sandro, 2001, D’Alessandro sandro, 2001, D’Alessandro

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SLIDE 15

CVM Assu

(D’Alessandro and

1)

Electric field intensificatio formation of upward leade

2)

Critical radius of 38 cm fr

a)

“Any sharp geometrical fea

a)

“Any sharp geometrical fea the critical value must be “

b)

“[T]he criterion for the init a stable upward leader is the critical radius”

3)

Ratio of velocity of downw is about 1.2

ssumptions

and Gumley, 2000) tion by structures affects ader from laboratory measurements

features with a radius of less that of features with a radius of less that of be “rounded off” to this value” nitiation of corona and consequently s the attainment of 3.1 MV/m at the

nward leader to upward leader

slide-16
SLIDE 16

CVM Assu

(D’Alessandro and

1)

Electric field intensificatio formation of upward leade

  • This is correct, from basic

ssumptions

and Gumley, 2000) tion by structures affects ader

ic freshman physics

slide-17
SLIDE 17

CVM Assu

(D’Alessandro and

2)

Critical radius of 38 cm fr

a)

“Any sharp geometrical fea critical value must be “rounde

  • Moore et al (2000) showed
  • Moore et al (2000) showed

much less than a few centi differently from those with

ssumptions

and Gumley, 2000) from laboratory measurements

features with a radius of less that the

  • unded off” to this value”

ed air terminals with radius of ed air terminals with radius of ntimeters behave quite ith radius of a few centimeters

slide-18
SLIDE 18

CVM Assu

(D’Alessandro and

2)

Critical radius of 38 cm fr

b)

“[T]he criterion for the init a stable upward leader is the critical radius” It is necessary for the field bet

  • It is necessary for the field bet

downward leader to be strong

  • No field measurements to confir
  • Becerra & Cooray (2007) mode

leader and found this not to be

  • “It is shown that the collection v

lightning protection areas of air

ssumptions

and Gumley, 2000) from laboratory measurements

nitiation of corona and consequently s the attainment of 3.1 MV/m at the between the “critical radius” and the between the “critical radius” and the

  • ng enough to sustain propagation

firm this

  • deled development of upward
  • be the case:

n volume concept overestimates the air terminals placed on complex structures”

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SLIDE 19

CVM Assu

(D’Alessandro and

3)

Ratio of velocity of downw about 1.2:1

ssumptions

and Gumley, 2000) nward leader to upward leader

  • During initial upward

leader, velocity ratio is about 10 to 1 about 10 to 1

  • Overall, velocity ratio

is about 3 to 1

  • D’Alessandro: “[A]

higher velocity ratio yields a smaller attractive radius

slide-20
SLIDE 20

CVM Assu

(D’Alessandro and

3)

Ratio of velocity of downw is about 1.2

  • During critical initial leade
  • f upward leader) velocity
  • This is when other objects

with the air terminal

  • D’Alessandro & Gumley (
  • “In fact, if one attempts to

does not have a real solution.”

ssumptions

and Gumley, 2000) nward leader to upward leader ader development (first 100 feet ity ratio is about 10:1

ts on the structure are competing

y (2001)

to use a ratio of 4 [or higher], Eq. (9) ution.”

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SLIDE 21

Field Validat

(Petrov & D’Ale (D’Alessandro an

  • Studies in Hong Kong and
  • Buildings protected by ER
  • Buildings protected by ER

according to CVM calcula

  • Claim to show protection
  • 2 to 15% of low intensity f

lightning protection system

ation of CVM

lessandro, 2000) and Petrov, 2006) and Kuala Lumpur, Malaysia ERICO Dynaspheres placed ERICO Dynaspheres placed ulations

  • n levels in the 85-98% range

ty flashed under 10 kA could bypass tem

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SLIDE 22

Field Validat

(Petrov & D’Ale (D’Alessandro an

  • Study in Kuala Lumpur
  • Data in study has been disp
  • Data in study has been disp

Lightning Research Pte. Ltd “This review shows that the fie

is invalid and should not be us

  • f air terminal placement.”
  • No independent verification of

ation of CVM

lessandro, 2000) and Petrov, 2006) sputed by Hartono & Robiah of sputed by Hartono & Robiah of

  • Ltd. of Kuala Lumpur

field data given in the above study used to validate the CVM method

  • f CVM method
slide-23
SLIDE 23

Field Validat

(Petrov & D’Ale (D’Alessandro an Two problems with methodolo

1)

Two different techniques

1)

Two different techniques with no way to differentia

2)

There was no control

ation of CVM

lessandro, 2000) and Petrov, 2006)

  • logy of field study:

es were tested with one study, es were tested with one study, tiate between the two

slide-24
SLIDE 24

Field Validat

(Petrov & D’Ale (D’Alessandro an

1)

Two different techniques way to differentiate betwe

  • Study used ERICO Dynas

CVM technique

  • If there was an effect, was

to the CVM?

ation of CVM

lessandro, 2000) and Petrov, 2006) es tested with one study, with no ween the two naspheres placed according to as it due to the Dynasphere or

slide-25
SLIDE 25

Field Validat

(Petrov & D’Ale (D’Alessandro an

ation of CVM

lessandro, 2000) and Petrov, 2006)

slide-26
SLIDE 26

Field Validat

(Petrov & D’Ale (D’Alessandro an

2)

There was no control

  • Only CVM placement wa
  • Only CVM placement wa
  • Would the results have be

placement method?

ation of CVM

lessandro, 2000) and Petrov, 2006) was tested. was tested. been different with another

slide-27
SLIDE 27

Field Validat

(Petrov & D’Ale (D’Alessandro an

  • Data from field study hav
  • If there were an effect, there is
  • If there were an effect, there is

was due to CVM or Dynasphe

  • No control
  • No independent verification of

ation of CVM

lessandro, 2000) and Petrov, 2006) ave been disputed.

e is no way to determine if the effect e is no way to determine if the effect phere

  • n of results
slide-28
SLIDE 28

Critique o

  • Lightning research does n

assumptions of CVM

  • No field study confirming

critical radius reaches 3.1 M

  • Contrary to laboratory studi

matter when smaller than c matter when smaller than c

  • Recent high-speed video is

that leader velocity ratios a

  • Problems with field verifi
  • Having only two field test

by proponents of CVM, is scientific consensus

e of CVM

s not support most of the

ng leader will develop when field at 3.1 MV/m tudies, field studies show radius does n critical radius n critical radius

  • is in conflict with the assumption
  • s are about 1:1

ification need to be resolved ests, with same methodology, , is not sufficient to meet

slide-29
SLIDE 29

Critique o

  • There is no consensus in t

CVM is valid

  • IEEE standards should be

by the scientific communi

  • It is premature to adopt CV
  • It is premature to adopt CV

e of CVM

n the scientific community that be based on principles accepted unity CVM into IEEE standard CVM into IEEE standard