Type 4: Outflow Boundary or Convergence Line intersecting the
                  Updraft region of a High-Precipitation (HP) Supercell


(1) One case supported this type of storm - mesoscale pattern.

hpstm.gif (38880 bytes)- External boundary
generated by convection to
the northeast of KLSX was
identified by:
  a) reflectivity fine line intersecting
  the inflow region (eastern flank)
  of a High-Precipitation (HP)
  Supercell.
  - warm season events
      1 evening.

 

 

Conceptual model of Type 4 severe wind MCS.


  - This type of storm reflectivity evolution is similar to those documented
     by Przybylinski and DeCaire (1985)  (Type IV) pattern, and
    Klimowski et al (2000) - northern High Plains.
    Additionally, Moller et al. (1990) has also documented this type
    of storm evolution across northern and central Texas.
                                                                 

-  An example of TYPE 4 pattern is shown in the 18 June 1998 event which
   occurred across eastern Missouri and parts of central and southern Illinois.

jun18r1.gif (53874 bytes)jun18r5.gif (57240 bytes)
     
0200 UTC 19 June 1998 reflectivity from KLSX. Image (left) is 1.5° slice. Image on (right) is
0.5° slice...zoomed 2x.

(a) The leading edge of the outflow generated by the convective line to
  the northeast is revealed by a reflectivity fine line.  This fine line
  intersected the HP storm's updraft  (storm's forward flank).
- Local vorticity residing within the external boundary appeared to be
  tapped by the  HP storm's updraft, resulting in the intensification of
  the storm's mesocyclone.

- Four-panel reflectivity / storm-relative velocity presentations of the
  HP storm is shown below.

                                        
jun18rv8.gif (48248 bytes)ju18rv10.gif (50033 bytes)

Four panel reflectivity / storm-relative velocity        Four panel reflectivity / storm-relative velocity
presentation at 0200 UTC 18 June 1998                    presentation at 0205 UTC 18 June 1998
(Upper two slices 1.5° / Lower two slices 0.5°)          (Upper two slices 1.5° / Lower two slices 0.5°)

(b) First (or Second) convective-scale circulation (mesocyclone
   core #1 or #2):
is often located along the HP storm's forward flank
   (storm's WER).
- Core #1 or #2 will often originate from 'mid-level beginnings'
   where updraft stretching causes the greatest cyclonic spin (vortex
   having 'descending characteristics.'   This is a key evolution
   in classifying this storm as a supercell  (per discussions with
   Burgess 1999).
- The storm-relative velocity imagery of the June 18, 1998 HP storm
   from 0200 and 0205 UTC showed an unbalanced velocity couplet
   (Circulation #2).
  The mesocyclone is located within the weak reflectivity notch
  (HP storm's eastern (updraft) flank). 

Rotational Velocity (Vr) trace of Mesocyclone core #2.

jun18c4.jpg (307831 bytes)

Rotational Velocity (Vr) Time-Height trace of the 2th circulation
18 June 1998. Magnitudes of Vr are in m/s.


- After Circ #2 reached it greatest height and strongest cyclonic
  shears at 0154UTC...reflectivity magnitudes along the line weakened
  as the line segment began to accelerate.  Rear Inflow notches,
  signifying entrainment of lower theta-e air were identified along
  the trailing flank of the northern part of the convective line.

-
First reports of damaging winds occurred across northern Washington
  county Missouri after 0205 UTC (south of the HP storm).
- It is common for swaths of damaging winds to occur immediately
  south of the HP storm and its associated mesocyclone (along the
  leading edge of the weaker reflectivity line segment.

- Tornadoes producing (F0 - F2 damage) may be associated
  with core #1 (or #2) or even subsequent cores.
 

- Vr magnitudes of Circ #2 intensified a second time within the
  1 and 3 km layer between 0210 and 0220 UTC (Vr = 18 - 20 m/s
  2-3 km layer) as the vortex continued to collapse.  Such
  intensification may enhance the downward transport of momentum
  from the storm's mid-level region to near the surface. 
 

jun18r26.gif (45300 bytes)jun18v26.gif (38974 bytes)

0215 UTC 18 June 1998 reflectivity (base velocity (right) from KLSX (0.5° slice).                                            

- Bowing of the convective line continued well through 0315 UTC
(75 to 120 km) southeast of KLSX.  Magnitudes of base velocity
exceeded 40 m/s over parts of southeast Monroe...southern St. Clair
...northern Randolph and western Washington counties in southwest
  Illinois.  Circ #2 weakened considerably at 0225 UTC...yet
  damaging winds continued through 0330 UTC (over 1 hour after
  the demise of the vortex).

jun18r30.gif (47881 bytes) jun18v30.gif (48146 bytes)

  0321 UTC 18 June 1998 reflectivity (base velocity (right)) from KLSX (0.5° slice).                                                


       

ju18xr30.gif (19739 bytes)ju18xv30.gif (19766 bytes)

0321 UTC 18 June 1998 reflectivity (base velocity) cross-sections from 0321 UTC 18 June 1998
from 120°/15 nm - 120°/72 nm.  

- A large swath of damaging winds occurred along the southern periphery
  of Circ #2 across northeastern Washington through the southern half of
  Jefferson county (south of STL) from 0204 through 0230 UTC and points
  further east and south across southwest Illinois.  (the greatest degree of
  damage occurred southeast of STL over southern St. Clair...northern
  Randolph and western Washington counties in southwest Illinois - estimated
  winds of 70 - 80 kts).
 

 
(2) SUMMARY:

- Of the 19 severe wind MCS events we surveyed, we were able to
  categorized 15 of them into four types (categories).  There were
  4 severe wind MCS events we placed in the 'OTHER' category.

- External boundaries or quasi-stationary frontal boundaries intersected
  a convective line in three of the four TYPES (categories)
  (Type 1- external boundary intersecting the northern end of the line
   segment; Type 2 - external boundary intersecting the central or south
   -central part of the line segment;  Type 4 - external boundary
  intersecting the updraft flank of an HP supercell). 

-
These boundaries appeared to have a role in the development of the
  first two convective-scale vortices associated with the system. 
  Our sample showed that the 2nd convective-scale vortex revealed
  stronger shears (Vr magnitudes) and greater depths compared to
  the first circulation.  The external boundaries appeared to serve as a
  source of local horizontal vorticity which aided in the development
  of the first two circulations.

- In 7 of the 15 cases surveyed (47%), weak F0 / F1 tornadoes
  were associated with the 2nd core.

- 3rd and subsequent circulations formed near the apex of the
  bowing structure south of the first and second cores.

- There were four events where the MCS did not intersect an external
  boundary or quasi-stationary frontal boundary.  Weak tornadoes
  occurred in two of the four events (due to an isolated cell - convective
  line mergers).  In the two tornadic cases, the depth of the cool layer
of air appeared to be quite shallow (less than 0.5 km deep).

- We were able to develop prelimiary conceptual models based on
  the cases studied.

  

(3) REFERENCES

 Burgess, D.W., R. R. Lee, S.S. Parker, D.L. Floyd, and D.L. Andra Jr., 1995:
      A study of mini-supercells observed by WSR-88D radars.   Preprints,
      27th Conf. on Radar Meteorology. Vail CO. Amer. Meteor. Soc.  4-6.
Houze, R.A., S.A. Rutledge, M.I. Biggerstaff, B.F. Smull, 1989:  Interpretation
      of Doppler weather radar displays of mid-latitiude mesoscale convective
      systems. Bull. Amer. Meteor. Soc., 6, 608-618.
Johns, R.H., and W.D. Hirt, 1987: Derechos: Widespread convectively induced
      windstorms.  Wea. Forecasting, 2, 32-49.
Maddox, R.A., L.R. Hoxit, C.F. Chappell, 1980:  A study of tornadic thunderstorm
      interactions with thermal boundaries. Mon. Wea. Rev., 108, 322 - 336.
Markowski, P.M., E.N. Rasmussen,  J.M. Straka, 1989:  The occurrence of
      tornadoes in supercells interacting with boundaries during VORTEX-95.
      Wea Forecasting, 13, 852 - 859.
Przybylinski, R.W., T.J. Shea, D.L. Ferry, E.H. Goetsch, R.R. Czys, and
      N.E. Wescott, 1993:  Doppler radar observations of High-Precipitation
      Supercells over the Mid-Mississippi Valley Region.  Preprints, 17th Conf.
      on Severe Local Storms. St. Louis, MO. Amer. Meteor. Soc., 158 - 163.
Rasmussen, E.N., and S.A. Rutledge, 1993:  Squall line evolution. Part 1:
      Kinematic and reflectivity structure. J. Atmos. Sci., 50, 2584-2606.
__________, J.M. Straka, R.P. Davies-Jones, C.A. Doswell III, F.H. Carr
      M.D. Eilts, and D.R. MacGorman, 1994:  The Verifications of the Origins
      of Rotation in Tornadoes Experiment: VORTEX. Bull. Amer. Meteor.
      Soc., 75, 997-1006.
Weaver, J.F., S.P. Nelson, 1982:  Multiscale aspects of thunderstorm gust
      fronts and their effects on subsequent storm development.   Mon. Wea.
      Rev., 110, 707-718. 
__________, and J.F.W. Purdom, 1995:  An interesting mesoscale storm-
      environmental interaction observed just prior to changes in severe
      storm behavior.  Wea Forecasting, 10, 449-453.
Weisman, M.L., 1993: The genesis of severe, long-lived bow echoes.
      J. Atmos. Sci., 50, 645-670.

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