43
1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning & Thunder

1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Embed Size (px)

Citation preview

Page 1: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

1. Hail growth; Thunderstorm electrification2. Cyclostrophic balance in tornadoes

Ahrens Chapter 7/8: Precipitation

Section on Hail

Chapter 14/15: Lightning & Thunder

Page 2: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Hail formation

• Starts with small ice crystal surrounded by abundant supercooled droplets – within a cloud with strong updraughts

• Growth by riming• Once initial crystal

shape is lost: graupel

Page 3: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Typical hail pellets~0.5 cm

Grapefruit-sized hailstones~10 cm

Serious Hazard

Page 4: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning
Page 5: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Hailstone structure

• Hail can grow quite rapidly (5-10 minutes)• As it grows, requires larger and larger updraught

velocities to support it• One path is approximately horizontally across

the cloud, growing as it traverses the updraught, then plummeting as it enters the downdraught

• Alternating light/dark layers due to different growth stages – dark layers have bubbles trapped; ‘wet’ growth vs ice (colder) growth

Page 6: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Cloud electrification

• Need a cold cloud – i.e. contains ice• Radar data indicates graupel or hailstones• As hail falls through cloud, bumping into

other cloud particles, it tends to become negatively charged

• Exact mechanism is not clear, but falling hail tends to make the lower cloud negatively charged, and leaves the upper part of the cloud positively charged…

Page 7: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Lowest part of cloudoften weakly positivelycharged

Page 8: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Lightning discharge

• Air has a low conductivity, but it can only cope with a gradient in charge (an electric field) up to ~106 volts per metre – beyond that it discharges: Lightning.

• 3 types of lightning:– 1a Within cloud– 1b Cloud to air– 2 Cloud to ground – most

energetic

Produce cloud flashes}

Page 9: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Lightning time sequence:1. Stepped Leader

Initial chargedistribution

Preliminarybreakdown inlower cloud – neutralizes the positive charge in cloud base

‘Stepped Leader’ advances in ~50 m steps, in 1 stime period between steps ~50 s

Downwards spread of negative charge induces a positive charge at ground

Page 10: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

2. Attachment and 1st Stroke

Stepped leadercontinues advance

When within ~10-100 m of the highest objects, a discharge moves up from the ground to meet the downwards advancing stepped leader

Once connected, large flow of electrons to ground – the ‘return stroke’- Intense flash

Page 11: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

3. Dart leader, subsequent strokes

New regions of negative charge in the cloud are connected

Dart leader moves down the mainpath followed by the first stroke, sending more electrons downwards

Further stroke;

Usually 3 or 4 strokes to discharge the cloud.Charge can build up again in as little as 10s

Page 12: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

NB Time-lapse photograph – many processes superimposed!

Can see a range of stepped leaders, together with the path of the main stroke (re-used for subsequent strokes)

Page 13: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Thunder• Return stroke raises air temperature in the channel it passes

through to >30,000K very quickly – air has no time to expand, so pressure rises, and air expands rapidly.

• Creates a shock-wave, which then creates a sound-wave a little further away: thunder

• Travels at speed of sound: 330 m s-1 (i.e. 1 mile in ~5 seconds)

• Stepped leaders also create thunder, but much less than the main stroke

• Sound waves tend to be refracted upwards, limiting the range over which thunder can be heard to within ~25 km of the source.

Page 14: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Days with thunder (1971-2000)

Page 15: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Distribution of lightning

Page 16: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Global Electrical Circuit

Thunderstormsare the ‘batteries’driving the circuit

Page 17: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Blue Jets, Red Sprites, etc.

These are allfairly recentlydiscovered electricalphenomena, closelyassociated withthunderstorms, that probably play a rolein the global electricalcircuit.

Page 18: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Summary

• Hail– Produced in cold clouds, multiple ascent and descent

cycles with growth by riming

• Lightning– Falling hail is negatively charged, leaving upper cloud

positive, lower cloud negative– Stepped leader; Return stroke; Dart leader;

subsequent strokes– Global electrical circuit driven by thunderstorms

• Thunder– Sound wave from 30000K heating by lightning stroke

Page 19: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Supercell, Kansas, rotating updraught

Page 20: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Supercell thunderstorms

• Rotating updraught– Rotation causes the storm to be more robust

– longer-lived, and therefore more dangerous

• Forms an area of low pressure at centre of rotation, called a mesolow

• Updraught centred on the low pressure

• Circulation around the low is in cyclostrophic balance…

Page 21: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Cyclostrophic balance

Acceleration (= Force/mass)given by: v2/r

v ~30 m s-1

r ~1000 m

v2/r ~0.9 m s-2

•Rotating air in a supercell generates an area of low pressure at the centre of the rotating updraught.

•The circulation is in ‘cyclostrophic balance’, where the pressure gradient force (PGF) is balanced by a centrifugal force

CentrifugalForce =

PGF

Lv

r

mv2

r

Tornado/supercellcase

Page 22: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Doesn’t this look a bit familiar?

CoriolisForce

PGF

Lv ~ 10 m s-1

Geostrophic Balance

r ~ 500 km

Centrifugal accelerationgiven by: v2/r

v ~10 m s-1

r ~500000 m

v2/r ~0.0002 m s-2

Centrifugal cceleration much smaller than the supercell case.

Coriolis force is due to planetary rotation

Centrifugal force is due to ‘local’ rotation

Large-scaleweathersystem

Page 23: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Coriolis Force

sin2f

Apparent force that acts on anythingthat moves in the Earth’s rotating frameof reference.

Coriolis parameter, f:

f is zero at equator, maximum at poles

mfvCF v = 10 m s-1

CF/m =0.0011 m s-2

At 50°Nf = 1.1 x 10-4 s-1

is the Earth’s rotation rate = 2 radians per day, or, in SI units (seconds): = 2 /(24x60x60) per second = 7.27 x 10-5 s-1

Page 24: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Comparing Coriolis & centrifugal forces

CoriolisForce

PGF

Lv ~ 10 m s-1

Geostrophic Balance

r ~ 500 km

Centrifugal accelerationgiven by: v2/r

v ~10 m s-1

r ~500000 m

v2/r ~0.0002 m s-2

Coriolis force is due to planetary rotation

Centrifugal force is due to ‘local’ rotation

Coriolis accelerationgiven by: fv

~0.0011 m s-2

Is bigger, but in some casesthe centrifugal acceleration isimportant at synoptic scales;But Ignore for now!

Page 25: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

CentrifugalForce =

PGF

Cyclostrophic balance

Lv

r

mv2Centrifugal accelerationgiven by: v2/r

v ~30 m s-1

r ~1000 m

v2/r ~0.9 m s-2

•Rotating air in a supercell generates an area of low pressure at the centre of the rotating updraught.

•The circulation is in ‘cyclostrophic balance’, where the pressure gradient force (PGF) is balanced by a centrifugal force

Coriolis accelerationgiven by: fv

~0.0033 m s-2

Is much smaller thancentrifugal: can ignoreCoriolis force for small scalerotations: storms/tornadoes

Page 26: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Summary of forces for rotating systems

• Supercell storms/tornadoes (~1 km across):– Cyclostrophic balance:– PGF vs. centrifugal force (ignore Coriolis)

• Synoptic weather systems (~1000 km):– Geostrophic balance:– PGF vs Coriolis Force (ignore centrifugal)

• Scale is all-important!

Page 27: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Back to Supercell storms

• Low pressure in rotating updraught can be so low that is causes saturation and forms a ‘funnel’ cloud

• (Drop in pressure is equivalent to ascent)

Page 28: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Tornadoes from supercell storms

Funnel cloud

Dust/debrisstirred upat surface

Pylonfor scale

Page 29: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Supercells & Tornadoes in the UK

• Generally much less severe than a typical US supercell/tornado, nevertheless…

• The UK experiences around 40 tornadoes a year – they generally do not cause damage, or are not even noticed

• A couple of recent cases:– 21st March 2004 – S. Midlands– 28th July 2005 – Lincolnshire– Data & images from www.torro.org.uk

Page 30: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Damage in Oxfordshire

Also accompanied by 2cm diameter hail

Page 31: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

UK supercell storm: 28th July 2005

Nottingham Skew T-log P – large CAPE

Path of two supercells:Right-moving is the strongest

Page 32: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Nr Peterborough, 28 July 2005

Page 33: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Damage nr. Peterborough

Page 34: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Farnborough, Dec. 2006

Page 35: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Spatial scale of storms

• Tornadoes are generally very localised, but can cause severe damage on small scales (100’s metres)

• Met: Weather and Climate (next semester), covers larger scale storms: tropical cyclones (hurricanes), also mid-latitude cyclones in more detail.

Hurricane Katrina, August 2005

Page 36: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

Analysis: 0000 Wed 11 Nov

Page 37: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

1200 Wed 11 Nov

Page 38: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

0000 Thu 12 Nov

Page 39: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

1200 Thu 12 Nov

Page 40: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

0000 Fri 13

Page 41: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

1200 Fri 13

Page 42: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

0000 Sat 14

Page 43: 1. Hail growth; Thunderstorm electrification 2. Cyclostrophic balance in tornadoes Ahrens Chapter 7/8: Precipitation Section on Hail Chapter 14/15: Lightning

1200 Sat 14