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