James G. LaDue, WDTB – FMI 2005

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Severe storm radar signatures

Jim LaDue

Warning Decision Training Branch,

NWS

Norman, OK

James.G.LaDue@noaa.gov

Topics

Estimating updraft strength

Mesocyclones

Assessing the potential for

Severe winds

Large hail

Tornadoes

Heavy rainfall

James G. LaDue, WDTB – FMI 2005

Updraft strength estimation

Upper level reflectivity core

Storm reflectivity and velocity structure

Low-level convergence

James G. LaDue, WDTB – FMI 2005

Elevated reflectivity core

Where does the precipitation form relative to the freezing level?

How high does the precipitation extend?

Link to loop

James G. LaDue, WDTB – FMI 2005

Case 1: July 10, 2003 very severe reflectivity profile

• Let’s examine the reflectivity profile of storm K0 and compare it to the

Severe Hail Index as determined by the previous page

James G. LaDue, WDTB – FMI 2005

Case 1: July 10, 2003 very severe reflectivity profile

0109 UTC

Deep, high reflectivity well

VIL = 83 kg/m 2

VIL density = 4.94 g/m 3

MEHS = 3” above/below

–20 

C level

-20° C

0° C

Z=55dBZ

Result: baseball hail

James G. LaDue, WDTB – FMI 2005

Case 1: July 10, 2003 very severe reflectivity profile

0109Z

Values are integrated upward

The Severe Hail

Index integrates the vertical reflectivity profile

Hail Detection

Algorithm

(HDA) converts this to estimated hail size

-20° C

0° C

Note how rapidly the SHI increases above the 0 °C level

POSH=90%

James G. LaDue, WDTB – FMI 2005

Case 2: July 10, 2003 Nonsevere updraft

• Let’s examine the reflectivity profile of storm F6 and compare it to the Severe Hail

Index as determined by the HDA worksheet

James G. LaDue, WDTB – FMI 2005

Case 1: July 10, 2003 nonsevere

0109 Z

Bottomreflectivity profile

Storm parameters for cell F6 heavy and weak

VIL = 42 kg/m 2

VIL density = 2.7 g/m 3

MEHS=.75” reflectivity

-20° C storm F6

0° C

Z=55dBZ

James G. LaDue, WDTB – FMI 2005

Case 1: July 10, 2004 nonsevere reflectivity profile

July 10, 2003

– Wichita

Storm parameters for cell F6

Note that SHI

VIL = 42 kg/m 2 responds

VIL density = 2.7 g/m 3

MEHS=.75” exponentially less given 10-

15 dBZ lower reflectivities in this storm

-20° C

0° C

POSH=90%

Result: no severe reports

James G. LaDue, WDTB – FMI 2005

Interim summary: updraft intensity through upper-level reflectivity

Use the higher slices to detect the towering cumulus above the boundary layer echoes

Look for the first strong core to develop above the freezing layer.

More severe storms have

• higher elevated reflectivities

• and more top heavy vertical reflectivity profile

Slightly smaller reflectivity aloft leads to large changes in expected weather

James G. LaDue, WDTB – FMI 2005

Severe updraft structural signatures

Objective : Understand how the following signatures are an indication of, or contribute to severe updrafts in convection

WERs

BWERs

Stormscale velocity

James G. LaDue, WDTB – FMI 2005

Nonsevere storm structure

Upper level storm top lies over lowlevel reflectivity maximum

Lower reflectivities overall

Low height of reflectivity thresholds

James G. LaDue, WDTB – FMI 2005

Severe sheared storm structure

Upper level storm top lies over lowlevel reflectivity gradient on the side of low-level storm relative inflow

Strong echo overhanging a

Weak Echo

Region (WER)

James G. LaDue, WDTB – FMI 2005

Trailing mesocyclone supercell updraft storm structure

Upper level storm top lies over lowlevel WER

Sometimes a

BWER (Bounded

Weak Echo

Region)

Sustained intense elevated reflectivity core

A mesocyclone

James G. LaDue, WDTB – FMI 2005

Severe sheared updraft intensity –

BWER detection

BWER (Bounded Weak Echo Region)

Needs a connection to the lowlevel WER

BWERs difficult to detect this far out

-20° C

Typical

BWER detection tops off near the

-20° C level

James G. LaDue, WDTB – FMI 2005

3.4°

2.4°

1.5°

0.5°

Classic severe updraft signature case

Trailing updraft

Normal width

Produced a few record sized hailstones

BWER = 2mi max size

-20° C

James G. LaDue, WDTB – FMI 2005

Severe updraft in a squall line segment

Squall line moving 52 kts

Storm top 26 kft AGL

Is there a

WER?

The ‘forward jump’ in the reflectivity from 2.4 to 3.4° is more than just movement between elevation slices

-20° C

James G. LaDue, WDTB – FMI 2005

Conceptual model of a more severe linear system updraft

Key things to note are the

Relatively nondescending RIJ

Front end echo overhang with linear BWER ahead of the surface gust front

Deep convergence zone

James G. LaDue, WDTB – FMI 2005

Updraft strength – Low-level convergence

Convergence parameters to affect updraft magnitude

• magnitude

• depth

• residence time of storm over convergence

James G. LaDue, WDTB – FMI 2005

Updraft strength – Low-level convergence depth

Assuming a steady state convergence

Depth:

Z = 2 km

Boundary width = 1 km (one .54 nm range gate)

Mean convergence over 1 km:



V = 10ms -1 / 1000m = .01 s -1

Updraft strength at 2 km W = (



V)

Z = .01s

-1 *2000m = 20 m/s

20 m/s

Convergence



V is simplified to be

V/width or

10 m s -1 /1000 m

6500ft - 2 km 1 km

10 kts (5 m/s)

James G. LaDue, WDTB – FMI 2005

Updraft strength – Low-level convergence depth

Assuming a steady state convergence

Depth:

Z = 3 km

Boundary width = 1 km (one .54 nm range gate)

Mean convergence over 1 km:



V = 10ms -1 / 1000m = .01 s -1

Updraft strength at 3 km W = (



V)

Z = .01s

-1 *3000m = 30 m/s

30 m/s

10 kts (5 m/s) 10000ft - 3 km

James G. LaDue, WDTB – FMI 2005

1 km

A severe upright convective system with deep, strong convergence

Deep Convergence zone

What do you think the spotter’s seeing?

15 kft

James G. LaDue, WDTB – FMI 2005

Conceptual model of a less severe linear system updraft

Key things to note are the

Descending RIJ

No deep convergence zone

Shallow sloping updraft over top of cold pool with numerous discrete cells merging into a line

James G. LaDue, WDTB – FMI 2005

Visual and radar obs of strong vs. weaker convective wind events

Case: 11 August

2004 Cocoa Beach,

FL

How deep is this gust front?

James G. LaDue, WDTB – FMI 2005

Visual and radar obs of strong vs. weaker convective wind events

Case: 11 August

2004 Cocoa Beach,

FL

How deep is this gust front?

James G. LaDue, WDTB – FMI 2005

Summary: Severe updraft signatures

• severe updraft signatures common to all storms in order of most severe first

BWER

WER

Intense reflectivity core, and deep relative to the –20

°

C level

Storm top displaced over WER

Deep convergence zone

James G. LaDue, WDTB – FMI 2005

Stormscale rotation

First, a review

Which is (cyclonic convergent, anticyclonic convergent, convergent, divergent)?

James G. LaDue, WDTB – FMI 2005

Mesocyclones

A Rankine Combined Vortex

James G. LaDue, WDTB – FMI 2005

Mesocyclone criteria

Core diameter from

–V max to +V max should not exceed 10 km

Rotational Velocity

Vr = (| –V max

| + | V max

|)/2 exceeds user thresholds

Persistence

10 min

Vertical continuity

V r -V max

+V max

James G. LaDue, WDTB – FMI 2005

mesocyclone

Rotational velocity = (|max outbound| + |max inbound|)/2

Use representative inbounds and outbounds, not the absolute maximum values

Meso diameter = 3.5 nm

Vmax = 50kt

Vmin = -22kt

Rotational V = 36 kt

James G. LaDue, WDTB – FMI 2005

Another classic supercell

James G. LaDue, WDTB – FMI 2005

J. LaDue

Another classic

James G. LaDue, WDTB – FMI 2005

J. LaDue

A diversity of mesocyclone sizes

All of these were tornadic.

Only the big one shows a meso hit

G. stumpf

Courtesy G. Stumpf

James G. LaDue, WDTB – FMI 2005

Summary: mesocyclones

Less than 5 nm, 10km in diameter

Persistent

Not shallow

Partly occupied by updraft and downdraft

Begins as mostly updraft then matures as downdraft forms

James G. LaDue, WDTB – FMI 2005

Severe weather threats

Wind

Hail

Tornado

Heavy rain

James G. LaDue, WDTB – FMI 2005

Severe wind threats

Isolated downbursts

Supercell wind threat

Organized multicell wind threat

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

The idea is to look for clues for potential downbursts before it reaches the ground.

Rapid and severe growth in updraft

Descent of the reflectivity core

Midlevel velocity convergence

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

Is this the time a warning should be issued?

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

As an aside

300 m

C Doswell

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

As an aside

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

This time height trend of reflectivity shows the descending core hitting the ground just after

0006 UTC.

Updraft phase

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

Updraft begins to build a core aloft

2356 UTC

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

0002 UTC

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

Midlevel convergence signifies downdraft commencing

0008 UTC

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

0014 UTC

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

Downdraft impacts the ground

0019 UTC

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

0024 UTC

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

0029 UTC

James G. LaDue, WDTB – FMI 2005

Visual and radar obs of a strong

Case: 12 August

2004 Cocoa Beach,

FL

Downburst precursor wind event

Mid altitude convergence is strong:

A downburst precursor

James G. LaDue, WDTB – FMI 2005

Visual and radar obs of strong wind event

• 5 minutes later…

James G. LaDue, WDTB – FMI 2005

Pulse storm downbursts

This event shows that VIL, height of Max reflectivity and storm top did not give lead time to downburst.

Tracking the descent of the core gave a better lead time

Monitoring updraft growth might give even better lead time

The stronger the elevated core, the stronger the initial updraft

James G. LaDue, WDTB – FMI 2005

Supercell severe wind threat

The most severe winds are in the Rear Flank

Downdraft (RFD) surrounding the mesocyclone.

Detected by deep convergence zone.

Pulse storm downburst mechanisms also occur

James G. LaDue, WDTB – FMI 2005

Supercell wind events

Can produce a large number of the most damaging wind events without tornadoes

Most common with

HP supercells

James G. LaDue, WDTB – FMI 2005

Rear flank downdraft contains the most intense winds but at this distance, 88D velocities overshoot highest winds.

Supercell wind events

3.4°

These high wind events often have a very deep convergence zone, extending 2 km or more.

Deep convergence zone

2.4°

15 kft

James G. LaDue, WDTB – FMI 2005

1.5°

0.5°

Organized multicell convective wind events

Squall lines

Bow echoes

James G. LaDue, WDTB – FMI 2005

Squall line heading toward radar

The worst winds are pointed directly at the radar. And the radar is close so that the low-level winds can be sampled.

James G. LaDue, WDTB – FMI 2005

Squall line not heading toward radar

Where do you think the strongest winds in this squall line will hit in the next hour?

James G. LaDue, WDTB – FMI 2005

Squall line not heading toward radar

James G. LaDue, WDTB – FMI 2005

Squall line not heading toward radar

• We must use other techniques to estimate wind severity

• Speed of motion

• Estimated strength of updraft

• Near storm environment

Radar sees only radial wind

True wind

Tangential wind component

James G. LaDue, WDTB – FMI 2005

Look for Mid Altitude Radial

Convergence Zone (MARC)

MARC signatures found within the strong cores

MARC signatures are small:

< 15 km long

> 25 m/s convergence

MARC signatures found here at

4 km AGL

James G. LaDue, WDTB – FMI 2005

Bow echoes

Narrow bow echoes are typically more severe than wide ones given everything else being equal.

Strongest winds

James G. LaDue, WDTB – FMI 2005

Bow echoes

Example of narrow bow echoes and very severe winds

James G. LaDue, WDTB – FMI 2005

Hail potential

Radar cannot directly detect hail

One big hailstone sends back the same energy as

1000s of regular raindrops

Either scenario could take place in a radar volume

Thus we have to infer the presence of hail from other clues

James G. LaDue, WDTB – FMI 2005

Favorable hail clues

Environmental

Dry air aloft, moist below, large instability

Enough wind shear for supercells

Fairly low freezing level (wet bulb) 7500-10000’

Storm structure

Intense reflectivity core (>55 dBZ) above the –20 C level

Strong updrafts with a WER or BWER

Storm rotation (supercells)

Updraft persistence

James G. LaDue, WDTB – FMI 2005

Favorable hail clues

Intense elevated core

Know how high your elevation slices are to your

0° and –20° C heights at the storm location.

Look for high reflectivity (>55 dBZ)

LRM products at 24 –

33 kft and especially the 33-60 kft level.

-20 C

0 C

James G. LaDue, WDTB – FMI 2005

Favorable hail clues

Bounded Weak Echo

Region (BWER)

Intense updraft forms a hole in the reflectivity core.

BWER

BWERs not typically seen this far out

Typical

BWER heights

3.4°

2.4°

1.5°

0.5°

James G. LaDue, WDTB – FMI 2005

Favorable hail clues

Weak Echo Region (WER)

Intense updraft also levitates a large

3.4° region of core.

Look for high over low reflectivities on the inflow side of a storm

2.4°

WER

A B

James G. LaDue, WDTB – FMI 2005

Watch out for anvil WERs.

WER typically from sfc to

15-20 kft.

They are not updrafts.

1.5°

0.5°

A

B

Vertically Integrated Liquid

Integrates what the radar thinks is liquid water in the vertical

Not a reliable hail indicator, no set thresholds

• Does show location of the ‘biggest storm’

James G. LaDue, WDTB – FMI 2005

VIL

Hail is loosely associated with VIL but the threshold changes with season and location

70

60

50 45

50

55

65 65 65

55

50

45

40

40

30

20

35

10

0

JAN FEB MAR APR MAY JUN JUL AUG SEP OCT NOV DEC

Month

James G. LaDue, WDTB – FMI 2005

40

VIL density

VIL is normalized by echo top height in meters and then multiplied by 1000 to yield a density of g/m 3

Attempts to reduce effects of different environments on a consistent large hail threshold

James G. LaDue, WDTB – FMI 2005

VIL = 47.5 kg/m 2

ET = 9.1 km

VIL = 70 kg/m 2

ET = 13.4 km

-20 C

0 C

VIL density

Warning performance statistics show a VIL density ~ 3.28 g/m 3 performs well as a large hail threshold in multiple

CWAs.

However…

Cerniglia and Snyder, 2002 – ER Tech memo

James G. LaDue, WDTB – FMI 2005

VIL density does not perform well in estimating severe hail size

Edwards and Thompson, 1998

James G. LaDue, WDTB – FMI 2005

VIL density

Other ordinary cell hail considerations

Reflectivities > 60 dBZ indicate a high likelihood of hail

Cannot discriminate hail size

The Hail Detection Algorithm tends to overestimate the Probability of Severe Hail

(POSH) in weakly sheared storms over low terrain

Hail potential increases as the freezing level approaches the ground or vice versa (i.e. topography)

James G. LaDue, WDTB – FMI 2005

Tornado potential

A tornado vortex signature

Strong gate-to-gate shear

Prefer to see this for at least two slices

The bottom should be on the lowest slice or within 600 m AGL

I prefer to see this persist for a couple scans

But some situations will not allow me to wait.

Due to beam spreading, my maximum TVS range is about 60 nm. After that, I’m only seeing mesocyclones.

James G. LaDue, WDTB – FMI 2005

Tornado vortex signature

Shear = |outbound + inbound| in adjacent gates

•Anywhere from 35 to more than 140 kts depending on range and severity

James G. LaDue, WDTB – FMI 2005

Occurrence of tornado with

LLDV

TVS low-level gate-to-gate velocity difference, LLDV (m/s)

James G. LaDue, WDTB – FMI 2005

LLDV m/s

FAR = green line

POD = red line

HSS = black line

Inset = POD vs FAR

Occurrence of tornado with MDV

TVS Maximum gate-to-gate velocity difference, MDV (m/s)

James G. LaDue, WDTB – FMI 2005

MDV m/s

FAR = green line

POD = red line

HSS = black line

Inset = POD vs FAR

A descending TVS

50% of are associated with supercells

(from Trapp et al., 1999)

Offers greater lead time

Trapp et al., 1999

James G. LaDue, WDTB – FMI 2005

Nondescending Tornado

Signatures

80% of squall lines

50% of supercells

(from Trapp et al., 1999)

James G. LaDue, WDTB – FMI 2005

What is the TVS seeing?

James G. LaDue, WDTB – FMI 2005

What is the TVS seeing?

1. Flanking line

1.

1.

James G. LaDue, WDTB – FMI 2005

What is the TVS seeing?

1. Flanking line

2. Dry slot and hook

1.

2.

1.

2.

James G. LaDue, WDTB – FMI 2005

What is the TVS seeing?

1. Flanking line

2. Dry slot and hook

TVS

Tornado

James G. LaDue, WDTB – FMI 2005

1.

2.

TVS

1.

2.

TVS

Example of a TVS in polar vs. cartesian coordinates

NIDS velocity

1 km boxes

Full resolution

SRM 0.2 km gates

June 13, 1998 OKC

James G. LaDue, WDTB – FMI 2005

Squall line vortices: 29 June

1998

Adapted from Pryzbylinski (2002)

James G. LaDue, WDTB – FMI 2005

Time height comparisons

Core #2 was more intense V r

=30 m/s

(60 kts)

Nondescending V r with time indicates low-level vorticity becoming stretched upward

Time-height V r trace Core #2.

James G. LaDue, WDTB – FMI 2005

Mesocyclone strength: isolated vs linear convection

Comparison of circulation characteristics between

Przyblynski et al. 2001 data set and Burgess et al. (1982) data set.

Larger mesocyclone diameters in linear systems than with isolated cell mesocyclones

Weaker V r with linear systems

Rot Vel

(m/s)

19.0 Squall

Line

(Low)

Trad

Super-cell

(Low)

Squall

Line

Trad

Supercell

23.0

18.8

25.0

Diameter

(km)

7.2

Height

(km)

5.4

7.4

6.0

7.6

9.2

L = surface to 8200 ft.

James G. LaDue, WDTB – FMI 2005

Nonmesocyclonic tornadoes

Considerations

Favored with steep 0-3 km lapse rates

0-3 km CAPE

Boundary with strong vertical vorticity

Slow moving boundary

Difficult to see on radar

James G. LaDue, WDTB – FMI 2005

Tornadoes in weak shear environments

Start with strong boundary with developing

CU

Boundary shear starts to roll into misocyclones

C

B

A

James G. LaDue, WDTB – FMI 2005

Tornadoes in weak shear environments

CU updrafts grow

Misocyclones A and B grow and move to the right while C weakens

C B

A

James G. LaDue, WDTB – FMI 2005

Tornadoes in weak shear environments

TCU continue to grow. Elevated core may form

Misocyclone B phases with one updraft forming a tornado

Misocyclone

A remains unattached, only dust devils form

C

B

A

James G. LaDue, WDTB – FMI 2005

Pre-existing vertical vorticity: a case

Storms moving with cold front

Outflow boundary moving down front

Rapid updraft growth on intersection

This cell motion tracked

Onset of elevated core indicating significant updraft

-20° C

0° C

James G. LaDue, WDTB – FMI 2005

Heavy rain producing storms

Rain rate is dependent on

Updraft strength X moisture content X efficiency

Total rainfall is dependent on

Rain rate

Motion

Size of storm along the motion track

• Let’s talk about a certain type of storm with high efficiency

Warm Rain dominated storm

James G. LaDue, WDTB – FMI 2005

Low topped heavy rainfall convection

09 June 2004

Very humid airmass

Lots of shear and low-level

CAPE

Not a lot of upper level

CAPE

James G. LaDue, WDTB – FMI 2005

Low topped heavy rainfall convection

09 June 2004

Reflectivity dominated by numerous small drops at observers location

James G. LaDue, WDTB – FMI 2005

An earlier warm rain dominated supercell on 09 June 2004

James G. LaDue, WDTB – FMI 2005

Cross Section through Warm-

Rain Supercell

Notice the reflectivity drop off above the freezing level.

James G. LaDue, WDTB – FMI 2005

Why spotters are still needed

VCP 11 or 21?

Aspect Ratio

Radar Horizon

James G. LaDue, WDTB – FMI 2005

Viewing Angle

Summary

Updraft strength

Stronger updrafts have any one of these features

Higher reflectivity at higher altitudes relative to the equilibrium level

Strong echo overhang,

• a BWER

Very strong and deep convergence zone

Not all of these must be present for a severe storm but if more exist, the more confidence you have of identifying a severe storm updraft

James G. LaDue, WDTB – FMI 2005

Summary continued

Mesocyclones

Must be persistent

Extend through > 2 km depth

Have time continuity

< 10 km wide

No minimum rotational velocity threshold

Mature mesocyclones can be divided between updraft and downdraft

James G. LaDue, WDTB – FMI 2005

Severe hazards

Severe winds

The strongest Individual downdrafts often follow strongest updraft signatures

Accompanied by Mid Altitude Radial

Convergence (MARC)

Often follow a deep convergence zone

Occur with small vortices such as mesocyclones

Keep in mind the favorable environments

(DCAPE, shear)

James G. LaDue, WDTB – FMI 2005

Severe hazards

Large hail

Intense upper-level updraft (-10 to -30

C layer)

Deep, intense reflectivities

WER

BWER (especially large ones)

Updraft persistence (indicated by a mesocyclone)

James G. LaDue, WDTB – FMI 2005

Severe hazards

Tornadoes

Mesocyclonic

Strengthening rotational velocity with strong low-level updraft signatures

Onset of a tornado vortex signature (TVS)

Onset of a hook

Squall line

Front inflow notch

Vortex rotational velocity increasing in intensity

Deep convergence zone

Nonmesocyclonic

Pre-existing source of vertical vorticity

Young but strong updraft

Favorable environment

James G. LaDue, WDTB – FMI 2005

Severe hazards

Heavy rain

Strong updraft is needed for inefficient storms

Weak updraft is enough if it is efficient

Large moisture

Slow motion

Large reflectivity core

Watch out for low topped warm rain events

James G. LaDue, WDTB – FMI 2005

resources

General radar interpretation - OKFIRST

• http://okfirst.ocs.ou.edu/train/materials/radar.html

NSSL mesocyclone and tornado case study page

• http://www.nssl.noaa.gov/wrd/swat/Cases/cases_pix.h

tml

NOAA radar page

• http://weather.noaa.gov/radar/

The Warning Decision Training Branch

• http://www.wdtb.noaa.gov/

James G. LaDue, WDTB – FMI 2005

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