A Detailed WSR-88D
Radar and Damage Survey
of a Severe Bow Echo Event on 14 June 1998
over the Mid-Mississippi Valley Region
Gary K. Schmocker
(Forecaster) WFO St. Louis
Ron W. Przybylinski (SOO) WFO St. Louis
1. Introduction
-
During VORTEX-95 P. Markowski, et
al. 1998 found that the majority of tornadoes in
supercell storms occurred near external,
pre-existing low level boundaries; usually
within 30 km of the boundary - on
the cool side where baroclinic horizontal vorticity
generation occurs.
- COMET Cooperative
project between WFO St. Louis and St. Louis Univ; in a number
of our cases, we found that quasi-stationary frontal
or pre-existing outflow boundaries
frequently intersected the northern end of convective
line segments. Short-lived
tornadoes often formed at the intersection (e.g. July
2, 1992; July 8, 1995).
- In this
presentation we will show:
- the affects of a pre-existing outflow boundary
which intersected a convective line;
- how it caused a dramatic change in the local
low-level wind shear profile
and appeared to aid in vortex
development.
- Although the radar detected fine line was moving quickly northeastward
(about 20
m/s), the absence of a relatively large and abrupt
pressure change on the WFO
St. Louis barograph trace lead to the conclusion
that this was an outflow boundary
rather than a gravity wave
Wind damage map across east central Missouri & southwest Illinois

- numerous reports
of wind damage (40-50 m/s peak gusts) between 1030 and 1300
UTC across east central Missouri and southwestern
Illinois including the northern
portion of the St. Louis metro area
- at least 3 non-supercell tornadoes (F0-F1)
- detailed storm survey by SOO, WCM and one forecaster revealed
classic intense
microburst damage patterns
2. Synoptic and Mesoscale Features

500 mb 1200 UTC June 14 1998
- 50 to 60 kt southwesterly wind max from Texas Panhandle
northeast into
central Missouri ahead of shortwave trough extending
from eastern Nebraska
southwest through the Texas Panhandle; this jet
streak was advecting dry
mid-level air into Missouri

Surface 1100 UTC June 14 1998
- warm front stretched from west central Missouri southeast
through northeastern
Arkansas; surface trough just north of warm front
from west central through southeast
Missouri; 64-70°F dewpoints across central and
southern Missouri along and south of a
line from MCI to STL

SGF 1200 UTC Sounding June 14 1998
- CAPE of 2006 J/Kg
- SR Helicity (0-2km) of 294 m2/s2
- pronounced drying between 800 and 600 mb
-
'Inverted V' structure (700 - 500 mb) signify damaging downburst potential.

KLSX WSR-88D VWP 1050-1137 UTC
- strong low-level wind shear (at least 20 m/s in the lowest 3
km) with strengthening and
increased veering of the winds between 0930 and
1130 UTC in the lowest 2 km
- rapid increase in the SR helicity (0-3km) between 1000 and 1130
UTC
- 0-2 / 0-3 km SR helicity increased from 340 (500) m2/s2 at 1025
UTC
to 670 (993) m2/s2 at 1111 UTC - near the time
of boundary passage at the radar site.
3. Initial Radar Analysis and MARC Signatures
0.5° reflectivity at 1030 UTC

- two parallel
lines of convection, oriented northeast-southwest, rapidly formed 90
to 120 km northwest of KLSX between 0900 and 1000 UTC
- the second line merged with the leading line after 1030 UTC
resulting in the
intensification of the leading convective line
- asymmetric structure of convective line
MARC Signatures and Wind Damage Plot

-2 MARC velocity signatures
identified
MARC #2 (291-301 radial) time-height plot

- second (and
strongest) MARC signature identified along the leading edge of
convective line at 1040 UTC, 11 minutes prior to time
of initial wind damage
across Montgomery county; MARC increased to a maximum
value of 35 m/s
(3.8 km height) at 1101 UTC during the time of wind
damage
- MARC magnitudes
identified in this case were not as strong or long lasting
as compared to other convective line cases we have
studied.
- a strong - persistent mesoscale RIJ current was not
observed in the SRM data;
- we have also noted that MARC is often not as easy to identify
with nocturnal
convection).
4. Circulation evolution near intersection of
convective line and
pre-existing outflow boundary
- after 1045 UTC, one convective cell along the
southwestern part of the leading
convective line intersected with a NW-SE outflow
boundary produced by an
earlier (0600-0900) MCS
0.5° reflectivity image at 1056 UTC

- note the weak convective cells oriented
northwest-southeast signifying the location of the
outflow boundary and intersecting the larger convective line to the northwest.
Circulation Track Map

- three
vortices rapidly formed just north of the intersection between the convective
line and the NW-SE outflow boundary (on the cool side
of the boundary)
with the second circulation (Circ #2) becoming the
strongest and longest lived.
Circulation #1 time - height trace

- Circ #1 formed at 1050 UTC in the region of the storm's inflow
notch.
- throughout much of its life cycle this circulation was
generally a shallow vortex
with the strongest cyclonic shears remaining in the
lowest 2 km.
4 Panel 0.5° & 1.5° reflectivity and SRM velocity images at 1101 UTC
depicting circs. #1 & #2

1111 UTC
4 panel 0.5° and 1.5° reflectivity and SRM velocity images

- Between 1101 and
1111 UTC, Circ. #2 intensifies as it moves eastward into Lincoln
county
- Circ. #2 remains located in the region of the storm's inflow
notch
- northeastward moving outflow boundary extends from inflow notch
in western
Lincoln county southeast to just east of KLSX at 1111
UTC
- convective line bowing just south of circ. #2
Circulation #2 time height section

- Circ. #2 initially formed below 2 km, rapidly intensified
within the lowest 2 km and
gradually deepened to an overall depth of 5 km midway
through its life cycle
- Circ. #2 lasted over one hour and spawned an F(0) tornado
- Circ. #2 appeared to aid in the acceleration of the bowing
segment south of the
vortex and helped to focus clusters of intense
damaging winds across the
northern parts of the St. Louis metro area
- strong circulations of this type, as well as other circs.
we have studied in past cases
appear to enhance the downward transport of
momentum leading to enhanced wind
damage south and southeast of the vortex
1131 UTC -
Six panel presentation of reflectivity / SRM images for 3.4, 2.4 and 1.5
degrees (left to right).

- the 1131 UTC 6 panel image shows the
overall reflectivity / SRM velocity structures.
Circ 2 is seen within the weak reflectivity notch / along the leading edge of the
convective line segment.
- Circ 2's strongest cyclonic shears remained within the lowest 2.5 km while overall core
diameter varied between 4 and 6 km.
- a strong gate-to-gate velocity couplet (delta V ~ 25 m/s) is observed at the lowest
slice. These very small couplets are frequently observed for only one or two volume
scans.
- the location of Circ 2 at and beyond 1131 UTC did not favor an optimum viewing angle,
thus Vr values were likely underestimated.
- the strongest degree of wind damage occurred just south of Circ 2.
5. Summary
a) The June 14th bowing MCS evolved in a
dynamic environment characterized by moderate instability and strong wind fields.
b) The MARC velocity signature was not as pronounced in this nocturnal event as compared to other
cases documented during the afternoon and early evening hours.
c) An outflow boundary orthogonal to the convective line was identified by small convective towers. 0-3 km SR helicity values significantly increased from 500 to 993 m2/s2 over a 45 minute period as the boundary traveled at 20 m/s over the KLSX radar site.
d) After 1050 UTC, three circulations formed near and north of the intersection of the external boundary and convective line. Circ #2, (a non-descending vortex) initially formed below 2 km, and appeared to aid in the acceleration of the bowing line segment south of the vortex.
e) Circ #2 along with other vortices we have studied in past cases appeared to enhance the downward transport of momentum leading to enhanced wind damage south and southeast of the vortex.
f) This case has shown that a boundary ('even a rapidly moving one') intersecting a convective line can augment the horizontal vorticity (SR helicity) leading to low-level mesocyclogenesis.
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