1 supercell thunderstorms adapted from materials by dr. frank gallagher iii and dr. kelvin...

60
Supercell Supercell Thunderstorms Thunderstorms Adapted from Materials by Dr. Frank Gallagher Adapted from Materials by Dr. Frank Gallagher III III and Dr. Kelvin Droegemeier and Dr. Kelvin Droegemeier School of Meteorology School of Meteorology University of Oklahoma University of Oklahoma Part III

Upload: austen-fleming

Post on 25-Dec-2015

225 views

Category:

Documents


0 download

TRANSCRIPT

Page 1: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

1

Supercell ThunderstormsSupercell Thunderstorms

Adapted from Materials by Dr. Frank Gallagher IIIAdapted from Materials by Dr. Frank Gallagher IIIand Dr. Kelvin Droegemeierand Dr. Kelvin Droegemeier

School of MeteorologySchool of MeteorologyUniversity of OklahomaUniversity of Oklahoma

Part III

Page 2: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

2

Importance of Storm-Relative Winds

Vorticity Vector

© 1990 *Aster Press -- From: Cotton, Storms

Play Movie

Storm-RelativeWinds

We obtain strong updraft rotation if the storm-relativewinds are parallel to the horizontal vorticity – or perpendicularto the environmental shear vector – this is easily determined

via a wind hodograph

Shear Vector

Page 3: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

3

Assessing S-R Winds

The degree of alignment between the storm-relative wind and the horizontal vorticity is critical for estimating the potential of an updraft to rotate

A particular tool – the wind hodograph – provides a simple graphical mechanism to assess this and other parameters

Page 4: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

4

Wind Hodograph A wind hodograph displays the change

of wind speed and direction with height (vertical wind shear) in a simple polar diagram.

Wind speed and direction are plotted as arrows (vectors) with their tails at the origin and the point in the direction toward which the wind is blowing. This is backward from our station model!!!

Page 5: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

5

Hodograph -- Example

Page 6: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

6

Hodograph

The length of the arrows is proportional to the wind speed. The larger the wind speed, the longer the arrow.

Normally only a dot is placed at the head of the arrow and the arrow itself is not drawn.

The hodograph is completed by connecting the dots!

Page 7: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

7

Hodograph -- Example

Page 8: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

8

SFC

500 m

1000 m

1500 m

2000 m

Hodograph -- Example

Page 9: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

9

Real Hodograph

Page 10: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

10

Hodograph Why Draw a Hodograph?

– Similar to a thermodynamic diagram – it makes life easier!

– We don’t have to look through a complex table of numbers to see what the wind is doing.

– By looking at the shape of the hodograph curve we can see, at a glance, what type of storms may form.

» Air Mass (garden variety) storms» Multicellular Storms» Supercell Storms» Tornadic Storms

– The shear on a hodograph is very simple to determine, as is the horizontal vorticity

– This allows us to assess helicity and streamwise vorticity

Page 11: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

11

Hodograph -- Example

Height (MSL) Direction Speed (kt)

250 m (SFC) 160 10

500 m 180 20

1000 m 200 35

1500 m 260 50

2000 m 280 75

Just by looking at this table, it is hard (without muchexperience) to see what the winds are doing and what

the wind shear is.

Page 12: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

12

Hodograph -- Example

Let us plot the winds using a station model diagram.

This is better but it is time consuming to draw and still is not that helpful. SFC

500 m

1000 m

1500 m

2000 m

Page 13: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

13

Hodograph -- Example Let us now draw the hodograph!

Let us draw thesurface

observation.160o at 10 kts

Since the windspeed is 10 kt,

the length of thearrow is only tothe 10 knot ring.

The directionpoints to 160o.

160

Page 14: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

14

Hodograph -- Example Let us now draw the 500 m observation.

Let us draw the500 m

observation:180o at 20 kts

Since the windspeed is 20 kt,

the length of thearrow is only tothe 20 knot ring.

The directionpoints to 180o.

Page 15: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

15

Hodograph -- Example We now place dots at the end of the arrows then erase the arrows.

Page 16: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

16

Hodograph -- Example We then connect the dots with a smooth curve and label the points.

SFC

500 m

1000 m

1500 m

2000 m

This is the finalhodograph!!!

Page 17: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

17

Hodograph -- Example What can we learn from this diagram?

– We see that the wind speeds increase with height.

» We know this since the plotted points get farther from the origin as we go up.

– We see that the winds change direction with height.

– In this example we see that the hodograph is curved and it is curved clockwise.

» If we start at the surface (SFC) and follow the hodograph curve, we go in a clockwise direction!

Page 18: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

18

Determining the Wind Shear– The wind shear vector at a given altitude is

tangent to the hodograph at that altitude and always points toward increasing altitudes

– The vector shear between two levels is simply the vector that connects the two levels

– Makes assessing the thermal wind vector (location of cold air) trivial!!

– The average shear throughout a layer is very useful in forecasting storm type

Page 19: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

19

SFC

1 km

2 km

3 km

Shear vectorat 2 km

Page 20: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

20

SFC

1 km

2 km

3 km

Shear vectorbetween

1 and 2 km

Page 21: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

21

SFC

1 km

2 km

3 km

Shear vectorbetween

sfc and 2 km

Page 22: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

22

Determining Horizontal Vorticity

– As shown earlier, the horizontal vorticity vector is oriented perpendicular and 90 degrees to the right of the wind shear vector

– This is very easily found on a hodograph!

Page 23: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

23

SFC

1 km

2 km

3 km

Horizontalvorticity vectors

Vertical windshear vectors

Page 24: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

24

Determining Storm-Relative Winds

– We can determine the S-R winds on a hodograph very easily given storm motion

– Storm motion is plotted as a single dot

Page 25: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

25

SFC

1 km

2 km

3 kmStorm Motion

(225 @ 30)

Page 26: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

26

SFC

1 km

2 km

3 km

Storm Motion Vector(225 @ 30)

Page 27: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

27

Determining Storm-Relative Winds

– We can determine the S-R winds on a hodograph very easily given storm motion

– Storm motion is plotted as a single dot– The S-R wind is found easily by drawing

vectors back to the hodograph from the tip of the storm motion vector

Page 28: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

28

SFC

1 km

2 km

3 km

Storm Motion Vector(225 @ 30)Storm-relative

winds can bedetermined at

any level, not just thosefor which observations

are available

Page 29: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

29

Use of Storm-Relative Winds

– Why do we care about the S-R winds?– Remember, only the S-R winds are

relevant to storm dynamics– In the case of supercell updraft rotation, we

want to see an alignment between the S-R winds and the horizontal vorticity vector

– This is easily determined on a hodograph

Page 30: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

30

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds can bedetermined at

any level, not just thosefor which observations

are available

Page 31: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

31

Importance of Storm-Relative Winds

Vorticity Vector

© 1990 *Aster Press -- From: Cotton, Storms

Play Movie

Storm-RelativeWinds

We obtain strong updraft rotation if the storm-relativewinds are parallel to the horizontal vorticity – or perpendicularto the environmental shear vector – this is easily determined

via a wind hodograph

Shear Vector

Page 32: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

32

Estimating the Potential For Updraft Rotation

– Ingredients» Strong storm-relative winds in the low-levels (at

least 10 m/s)» Strong turning of the wind shear vector with

height (90 degrees between the surface and 3 km)

» Strong alignment of the S-R winds and the horizontal vorticity – to develop rotating updrafts

» All of this can be quantified by a single quantity- the Storm-Relative Environmental Helicity

Page 33: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

33

Storm Relative Environmental Helicity

SREH -- A measure of the potential for a thunderstorm updraft to rotate.

SREH is typically measured over a depth in the atmosphere:– 1 to 3 km– 0 to 4 km

A good helicity estimate depends on accurate winds and storm motion data

Page 34: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

34

Storm Relative Environmental Helicity

SREH is the area swept out by the S-R winds between the surface and 3 km

It includes all of the key ingredients mentioned earlier

It is graphically easy to determine

Page 35: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

35

Storm Relative Helicity180

270

Storm MotionSFC

1 km

2 km

3 km4 km

5 km6 km

7 km

This area representsthe 1-3 km helicity

SREH Potential Tornado Strength

150 - 300 m2 s-2 Weak

300 - 500 m2 s-2 Strong

> 450 m2 s-2 Violent

Page 36: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

36

Typical Single-Cell Hodograph

Weak shear, weak winds

Page 37: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

37

Typical Multicell Hodograph

Somewhat stronger winds and shear, with S-R winds providing mechanism

Hodograph is essentially straight, especially at low levels

Page 38: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

38

Typical Supercell Hodograph

Strong wind, shear vector turns with height, strong S-R winds

Note curved shape of hodograph at low levels

Page 39: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

39

SFC

1 km

2 km

3 km

Storm Motion Vector(225 @ 30)

Which Storm Motion Produces a Strong, Cyclonically-Rotating Supercell?

Page 40: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

40

Estimating the Potential For Updraft Rotation

– Ingredients» Strong storm-relative winds in the low-levels (at

least 10 m/s)» Strong turning of the wind shear vector with

height (90 degrees between the surface and 3 km)

» Strong alignment of the S-R winds and the horizontal vorticity – to develop rotating updrafts

Page 41: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

41

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds

Speed of S-R WindsAlignment of S-R Winds and Vorticity

Page 42: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

42

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds

Storm-Relative Environmental Helicity

Page 43: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

43

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds

Speed of S-R WindsAlignment of S-R Winds and Vorticity

Page 44: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

44

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds

Speed of S-R WindsAlignment of S-R Winds and Vorticity

Page 45: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

45

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds

Storm-Relative Environmental Helicity

Page 46: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

46

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds

Speed of S-R WindsAlignment of S-R Winds and Vorticity

Page 47: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

47

SFC

1 km

2 km

3 km

HorizontalVorticity vectors

Storm-relativewinds

Storm-Relative Environmental Helicity

Page 48: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

48

SFC1 km

2 km3 km

Making an Optimal Hodograph

Page 49: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

49

SFC1 km

2 km3 km

Making an Optimal Hodograph

Note unidirectional shear, butGround-relative winds veer with height

Page 50: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

50

SFC1 km

2 km3 km

Making an Optimal Hodograph

HorizontalVorticity vectors

Page 51: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

51

SFC1 km

2 km3 km

Making an Optimal Hodograph

HorizontalVorticity vectors

Place the stormmotion to get a

strong cyclonic supercell

Page 52: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

52

SFC1 km

2 km3 km

Making an Optimal Hodograph

HorizontalVorticity vectors

Change the hodograph toobtain a strong supercellgiven this storm motion

Page 53: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

53

SFC1 km

2 km3 km

Making an Optimal Hodograph

HorizontalVorticity vectors

Change the hodograph toobtain a strong supercellgiven this storm motion

Page 54: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

54

SFC

1 km

2 km3 km

Making an Optimal Hodograph

HorizontalVorticity vectors

Page 55: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

55

SFC

1 km

2 km3 km

Making an Optimal Hodograph

HorizontalVorticity vectors

Storm-relativewinds

Page 56: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

56

Predicting Thunderstorm Type: The Bulk Richardson Number

Need sufficiently large CAPE (2000 J/kg) Denominator is really the storm-relative inflow kinetic energy (sometimes called the BRN Shear) BRN is thus a measure of the updraft potential versus the inflow potential

2S

CAPEBRN

25006000

2 )(2

1uuSwhere

Page 57: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

57

Results from Observations and Models

Page 58: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

58

General Guidelines for Use

40035

505

BRNforMulticells

BRNforSupercells

Page 59: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

59

Page 60: 1 Supercell Thunderstorms Adapted from Materials by Dr. Frank Gallagher III and Dr. Kelvin Droegemeier School of Meteorology University of Oklahoma Part

60