Title: Severe Storm Structures
1Severe Storm Structures
- Clark Evans
- Current Weather Discussion
- 26 March 2008
2Goals and Outline
- To be able to identify conditions favoring linear
versus discrete storms - To be able to identify and analyze a multitude of
linear convective systems - To better understand supercells and supercellular
structures, including left- and right-moving
storms
3Linear and Discrete Modes
(image courtesy NWS Southern Region)
- Linear an organized set of strong to severe
storms often taking a linear shape - Examples squall line, derecho, mesoscale
convective system (MCS), etc.
4Linear and Discrete Modes
(image courtesy Univ. of Oklahoma)
- Discrete an individual, often supercellular
storm. Has a uniquely identifiable updraft and
storm structure, potentially including forward
and rear flanking downdrafts. - Associated with the most prolific tornado
outbreaks
5Linear and Discrete Modes
- What atmospheric characteristics distinguish
between conditions favorable for discrete versus
linear storms? - What atmospheric characteristics promote the
upscale development from discrete storms to
linear features?
6Linear and Discrete Modes
- Factors that are important for determining storm
mode include - Type of focusing mechanism
- Strength of upper-level forcing
- Strength of capping, if any
- Orientation of wind fields with respect to
large-scale boundaries - Time of day?
- and perhaps more.
7Linear and Discrete Modes
- Which of these boundary types favor discrete
storm development? - Which of these boundary types favor linear storm
development?
8Linear and Discrete Modes
- Generally, it is tied to the other environmental
factors at play for each type of boundary - Capping
- Strength of large-scale forcing
- Upper level wind fields
- That said, each boundary type does have
distinguishing characteristics for storm mode
9Linear and Discrete Modes
- Cold frontsoften linear
- Sharply sloped
- Often near strongest upper level forcing
- Warm frontsdiscrete potential
- Not sharply sloped
- Usually weaker upper level forcing
- Dry lines and pre-frontal troughsdepends
- Capping often plays a role
- If capping is broken or weak, magnitude of upper
level forcing plays a role
10Linear and Discrete Modes
- A closer proximity to upper level forcing often
leads to a greater linear storm threat - Associated with very strong height falls,
vorticity advection and/or upper level
divergence/diffluence - Found with very strong low level convergence
along a boundary - Subsequent large-scale lift often completely
erodes any cap that was in place - Colder mid-level temperatures enhance instability
- Vertical wind profile tends to become more
unidirectional, leading to straight-line
hodographs and favoring lines - Often found in conjunction with sharp focusing
mechanism, leading to large-scale storm and
updraft development
11Forcing and Focusing Example
- Left 500 hPa analysis
- Right Surface analysis
- Both from 0000 UTC 6 February 2008, courtesy SPC
12Forcing and Focusing Example
- Closer to the stronger upper-level forcing and
sharper surface boundary linear - Further away in free warm sector along
pre-frontal wind shift discrete
Radar mosaic at 2234 UTC 5 February 2008 Courtesy
Storm Prediction Center
13Linear and Discrete Modes
- Discrete modes are favored when there is some
capping in place - What is too much capping? Somewhat subjective and
depends on the situation. - Need sufficient surface-based heating coupled
with synoptic-scale and mesoscale lift to erode
cap locally - If synoptic-scale lift and forcing are too
strong, cap may be broken everywhere all at once,
thus favoring linear development
14Capping Erosion Example
- Lake Charles, LA soundings, courtesy SPC
- Left 1200 UTC 5 Feb Right 0000 UTC 6 Feb. 2008
15Capping Erosion Example
- Combination of surface-based heating plus
large-scale lift helped erode the cap during the
day on 5 February 2008 - Coupled with subtle pre-frontal wind shift
focusing mechanism and distance from upper level
forcing, discrete activity took place! - Do recall, though, that wind shear and
instability parameters for severe convection must
still be met despite distance from upper level
forcing!
16Capping Erosion Example
- Del Rio, TX soundings, courtesy SPC
- Left 1200 UTC 4 May Right 0000 UTC 5 May 2007
17Capping Erosion Example
- Strong surface-based heating helped put a dent in
the cap - but, weak synoptic-scale forcing and lift only
minimally lifted the cap - Thus, the cap remained in place and storm
development did not occur (independent of extreme
instability and weak shear)
18Linear and Discrete Modes
- Structure of the deep layer wind field can be
important in determining storm mode. - Primarily arises out of consideration for
hodograph structure and orientation to any
focusing mechanisms. - There is no set rule of thumb that works for
all situations and types of boundaries, however.
19Linear and Discrete Modes
- Generally speaking, greater directional shear
leads to a greater discrete storm potential
(left). - Weaker directional shear straight-line
hodographs leads to a greater linear storm
potential (right).
20Linear and Discrete Modes
- Storms that can ride the warm front have the
potential to be long-tracked tornado producers
(left) - Storms that are directed across the warm front
become elevated and occasionally linear, negating
the tornado threat (right)
21Linear and Discrete Modes
- Time of day plays a minor role in determining
storm mode. - Generally speaking, if storms form before the
boundary layer decouples, discrete activity is
more likely. - Before sunset or generally shortly thereafter
- Decoupling favored under relatively light winds
or strong radiational cooling conditions - Storms forming or lasting after this are more
linear.
22Linear and Discrete Modes
- As instability weakens after sunset, storms can
have a harder time maintaining their updrafts. - Downdrafts thus dominate
- Cold pool generation leads to storms becoming
outflow dominant - New storms can form along outflow boundary,
leading to upscale growth - If atmospheric conditions are ripe, this upscale
growth can lead to an MCS, squall line, or
derecho - Need sufficient shear, low-level instability, and
forcing moving in conjunction with convective
system
23Linear and Discrete Modes Summary
- Dependant upon the interaction of many factors.
- Discrete modes are favored
- During the daytime away from the strongest
upper-level forcing - With greater directional shear values
- Away from the sharpest focusing mechanisms
- In regions of some capping
- Linear modes are favored
- Closer to well-defined focusing mechanisms
- Closer to stronger upper level forcing and weaker
directional shear - In regions of weak to no capping
- They are also favored at night as discrete
convection grows upscale.
24Linear Convective Systems
- Linear convective systems come in all shapes and
sizes and are referenced with numerous terms - Mesoscale convective systems
- Squall lines and bow echoes
- Derechos
- Quasi-linear convective systems (QLCS)
- Line echo wave pattern (LEWP)
25Mesoscale Convective Systems
- Generic term for any organized convective feature
on the mesoscale - Characterized by a descending rear inflow jet
(notch) on velocity (reflectivity) radar imagery - Driven primarily by buoyancy and strong
upper-level divergence
26Mesoscale Convective Systems
- Often characterized by circular appearances on
satellite imagery with cold cloud tops - Can lead to the formation of a mesoscale
convective vortex (MCV) at mid-levels
(image courtesy NWS WFO No. Indiana)
27Mesoscale Convective Systems
- What are the factors used to diagnose MCS
longevity? - Maximum shear in 0-1 and 6-10 km layers
- Mid-level lapse rates
- Most unstable CAPE
- Mean winds above the boundary layer
- In general, higher is better for each parameter.
- Resource Coniglio and Corfidi (2006)
28Mesoscale Convective Systems
- MCS features both development and longevity
are not well-handled by models - Large-scale models cannot represent cold pool
generation and propagation - Mesoscale models often either way too strong and
fast or dont show any development at all - Non-horizontal resolution problems include
- Convective parameterizations
- Boundary layer parameterizations
- Microphysics parameterizations
- And more
29Squall Lines and Bow Echoes
- Multicell complex of strong to severe storms
- Leading edge buoyancy driven, strongest
convection - Back edge trailing stratiform region, where
storms go to die - Generally strongest on the southern edge of its
forward bulge - Tail-end Charlie structures as well
(image courtesy theweatherprediction.com)
30Squall Lines and Bow Echoes
- Four primary types of squall lines
- Broken line generally occurs along some focusing
mechanism - Back building training storms gradually grow
into a line, often with mean winds parallel to
the focusing mechanism - Broken areal upscale growth of discrete
convection - Embedded areal linear growth as a result of
elevated instability, either upright or slantwise
31Squall Lines and Bow Echoes
- Longevity and severity dependent upon
- Instability, surface-based or elevated
- Proximity and magnitude of upper-level forcing
(closer or stronger is better) - Ability to generate or transfer momentum to the
surface - Mid-level dry air generation
- Strong upper-level winds transport
- Can last well beyond the point the severe threat
ends/diminishes
(image courtesy theweatherprediction.com)
32Squall Lines and Bow Echoes
- Common features of bow echoes are book end
vortices - Mesocyclone vortices that form along curving ends
of the bow echo - Northern one can lead to tornado formation with
cyclonic rotation
(image courtesy NWS Western Region)
33Derechos
- Intense, often long-lived squall lines
- Technical definition a widespread and long
lived windstorm that is associated with a band of
rapidly moving showers or thunderstorms. - Come in two types
- Serial
- Progressive
(image courtesy NWS WFO Louisville, KY)
34Derechos
- Serial derecho extensive squall line with
multiple embedded bow echoes - Progressive derecho smaller-scale, often
associated with just one bow echo
(images courtesy NWS WFO Louisville, KY)
35Derechos
- Most prevalent during summer under ring of fire
scenarios - Shortwave disturbances around periphery of
subtropical ridge ignite convection - Moderate shear plus extreme instability leads to
organization and growth of derecho structure
36Quasi-linear Convective Systems
- A type of forward propagating MCS
- Similar to a squall line or derecho in structure
and evolution - Convection takes on the structure of a line with
embedded discrete elements
(image courtesy NWS WFO St. Louis, MO)
37Quasi-linear Convective Systems
(image courtesy NWS WFO St. Louis, MO)
- Semi-discrete elements within the QLCS often are
accompanied by mesovortices and weak tornadoes - Associated with MARC (Mid-altitude radial
convergence) signatures in velocity data - Key attribute rear inflow jet of 25 m s-1
- Form under conditions that have ambiguous signs
for ultimate storm mode hybrid conditions
38Line Echo Wave Pattern
- Characterized by an S shape on radar
- Takes on the appearance of a mesolow with
meso-warm and cold fronts - Southern bow echo enhanced wind damage potential
- Mesolow region enhanced low-level shear and
tornado potential
(image courtesy Texas AM Univ.)
39Splitting Storms and Storm Propagation
- What are the atmospheric conditions that promote
storm splitting? - What conditions favor the right splits?
- What conditions favor the left splits?
- What influences both discrete and linear storm
motion?
40Storm Splitting
- Storms split due to non-linear supercellular
dynamics! - Updrafts tilt vorticity into the vertical,
resulting in horizontal circulations on either
side of the updraft - Pressure perturbations are proportional to these
circulations (p -?2) - Rising motion is favored with pressure
perturbations - In the vicinity of the updraft weaker motion,
corresponding to our split region!
41Storm Splitting
- Generally, the right split is favored.
- This is due to advection of the updraft by the
shear vector and the resultant pressure
perturbations within the supercell. - This arises out of cyclonic shear profiles.
- Tends to be those most associated with
mesocyclone and tornado development! - Left splitting storms often rapidly weaken under
most conditions.
42Right Split Hodograph
Note well-defined cyclonic curvature in storm
layer.
43Storm Splitting
- Left moving splits are favored with
counterclockwise shear profiles. - Hodographs either curve entirely or partially
counterclockwise - Concordant with backing of the vertical wind
profile at a location - Oftentimes such storms are elevated in nature and
rarely tornadic - Such conditions are seen approximately 10 of the
time
44Left Split Hodograph
Note anticyclonic curvature between 550-700 hPa
(example courtesy James McCormick)
45Storm Motion
- Two main factors
- Mean deep-layer (roughly 0-6 km) wind
- Deep-layer shear vector
- Linear storms generally move along the mean wind
and deep layer shear vectors - Discrete storms generally move in the same
direction with a disposition to move to the right
for right moving storms
46Storm Motion Example
47Where Weve Been
- With severe storms, weve already covered a lot
- One case study (5 February 2008)
- Sounding analysis for severe storms
- Synoptic-scale severe forecasting and analysis
- Storm modes, including supercell structures and
linear convective systems
48Whats Still to Cover?
- Theres still a bit more to take into account,
however - Radar analysis rotation, convergence,
divergence, elevated vs. low-level signatures,
etc. - More real-life examples in-class exercise,
putting everything together - Well get into these in the next few weeks.