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Richard Sonnenfeld Physics Department & Langmuir Laboratory for Atmospheric Physics New Mexico Institute of Mining and Technology (Photo courtesy of Harald Edens) Understanding the Lightning Leader APS 4Corners 10/22/2011 Abstract P1.00001 (1:30 pm) 1

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Richard Sonnenfeld

Physics Department & Langmuir Laboratory for Atmospheric Physics

New Mexico Institute of Mining and Technology

(Photo courtesy of Harald Edens)

Understanding the Lightning Leader

APS 4Corners 10/22/2011

Abstract P1.00001 (1:30 pm)

1

Lightning statistical parameters● 40 flashes/second on Earth.● I_peak=100,000 amps● V_cloud=30 Megavolts● Arc Temperature = 10,000 K● Charge transfer Q=20 coulombs● Max dI/dt ~ 10^11 Amps/s● Channel radius r ~ 1 cm● Stepped Leader velocity <0.001c● Dart Leader velocity 0.1c● Return Stroke velocity 0.5c

(Photo courtesy of Harald Edens)

(From Uman, “All AboutLightning “)

(NASA Photo)

2

There are only two things to study about lightning physics …

3

There are only two things to study about lightning physics …

Charging andDischarging

4

Charging● How are charges distributed in storms?

● How are charges created on hydrometeors?

– Cloud physics – freezing processes● What is link between lightning and severe weather?

– Updrafts, fronts, supercells

– Hurricanes / tornadoes / volcanoes● How is lightning linked to climate?

– Land / ocean differences

– Seasonal variations

5

Electrical structure of stormsCharging

6

∇⋅E⃗=ρϵ0

ρ=ϵ0ΔEΔ z

ρ=ϵ0+60kV /m1000m

∼0.5nCm3

Charging

7

Charges separate because

Of different terminal velocities.

Updrafts feed moisture into

The freezing zone and drive

Collisional charging

Charging

7 a

Charging is driven by updrafts – Linked to severe weather (tornadoes, hurricane eye-walls)

8

Discharging● What is the speed of a leader (in the

clouds)● What is the current in a leader?● What is the charge on a length of channel?● How does leader stay hot

9

● Streamers● Tendrils of ionized air● Cold processes● Driven by electric field, impact and

photo-ionization..● Quenched by recombination.

EB∼3 (MV /matm

)×p (atm)

10

Leaders● Are low current

(100 Ampere) arcs.● Streamers keep

leaders hot.● Leaders are nearly

equi-potentials.● Positive leaders move

smoothly.● Negative leaders step,

and are RF noisy.

11

Leader – Arc properties

● Balance self-heating,

Conductive cooling,

Recombination rate.

12

B

A

Discharging● What is the speed of a leader (in the

clouds)● What is the current in a leader?● What is the charge on a length of channel?● How does leader stay hot

13

Instruments

● Lightning Mapping Array.● Electric field sonde.● High Speed Video

14

Discharging● What is the speed of a leader (in the clouds)● What is the current in a leader?● What is the charge on a length of channel?● How does leader stay hot

16

– 10,000 Samples/s– 16-bits/Sample,– Measure 8 channels

● E-field (Channels 0-3)● Timing (Channel 4)● B-field (Channels 5-7)

A vector field-change sonde

17

BA

Modeling – TDMD method

18

A

B

Modeling – TDMD method160 km/s

100 km/s

19

DC

-0.5 mC/m

-2.4 mC/m-1.1 mC/m

20

DC

Modeling – TDMD method● “Time-dependent, multi-dipole”● RF emissions are assumed to be associated with

charge movement.● A negative charge is assumed to be deposited at the

location of the latest RF source.● A positive charge is placed on some previous source to

give the best-fit to the electric field change.

21

Modeling – TDMD method

22

Discharging● What is the speed of a leader (in the clouds)● What is the current in a leader?● What is the charge on a length of channel?● How does leader stay hot

23

Lightning passes 200 m from ESonde

24

Horizontal E-fields show negative charge passing by and creating

new leader

25

26

27

Step-recoil waveClockwise

“C” on vector

plot shows negative chargemoving towardright

28

Step-recoil wave

CCW “C” on vector

plot shows positive chargemoving toward

left

29

Step-recoil wave

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Triggered Lightning

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091,564 us

112,657 us

32

Triggered Lightning

116,563 us

33

Triggered Lightning

120,157 us

34

Triggered Lightning

122,813 us

35

Triggered Lightning

122,969 us

36

Triggered Lightning

129,688 us

37

Triggered Lightning

129,844 us

38

Triggered Lightning

130,000 us

39

Triggered Lightning

130,156 us

40

Triggered Lightning

Integrated High-Speed Video

41

Luminosity vs. Channel

42

Summary and Conclusions● Currents on leaders in clouds are in hundreds of

amperes (in contrast to tens of thousands in CG)● Leaders in the clouds move very slowly (about

10^5 m/s)● Leaders seem to create recoil waves as they step

forward. These waves are required by charge conservation and also probably help keep channel hot.

● Channels in intracloud lightning seem to act independently

● The wonderful complexity of natural lightning is beginning to yield to study by coordinated techniques.43

Supporting slides ...

Modeling – TDMD method

35

Currents, Fields, and Energy in an IC leader

36