A COMPARISON OF VERTICAL MOTIONS OBTAINED FROM DIFFERENT FORMS OF THE OMEGA EQUATION Christopher J. Melick and Phillip J. Smith Department of Earth and Atmospheric Sciences Purdue University West Lafayette, Indiana - PowerPoint PPT Presentation

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A COMPARISON OF VERTICAL MOTIONS OBTAINED FROM DIFFERENT FORMS OF THE OMEGA EQUATION Christopher J. Melick and Phillip J. Smith Department of Earth and Atmospheric Sciences Purdue University West Lafayette, Indiana

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Title: A COMPARISON OF VERTICAL MOTIONS OBTAINED FROM DIFFERENT FORMS OF THE OMEGA EQUATION Christopher J. Melick and Phillip J. Smith Department of Earth and Atmospheric Sciences Purdue University West Lafayette, Indiana


1
A COMPARISON OF VERTICAL MOTIONS OBTAINED FROM
DIFFERENT FORMS OF THE OMEGA EQUATIONChristopher
J. MelickandPhillip J. SmithDepartment of
Earth and Atmospheric SciencesPurdue
UniversityWest Lafayette, Indiana
2
OBJECTIVE
  • Comparison of vertical motions obtained from
    Four quasi-geostrophic (QG) forms and one
    ageostrophic form (extended) of the omega
    equation.
  • Case study Strahl and Smith (MWR2001)
  • Explosive cyclone development accompanied by
    upper-air wave merger over North America (Nov.
    2-3 1999)

3
INTRODUCTION
  • Scale Analysis
  • V 10 m/sec
  • W 1 cm/sec
  • ?Too small to be measured directly.
  • ?Computational methods required.
  • NOTE Assumes synoptic-scale (large spatial and
    temporal) conditions.

4
COMPUTATIONAL TECHNIQUES
  • Kinematic Integrated Divergence/Convergence in
    Continuity Equation
  • Vorticity Integrated Vorticity
    Advection/Tendency
  • Adiabatic Temperature Advection/Tendency
  • Isentropic Pressure Advection along Potential
    Temperature Surface
  • Omega Equation Combine Vorticity Equation and
    1st Law of Thermodynamics

5
QG THEORY
  • Ageostrophic motions and hence vertical motions
    are produced as the atmosphere progresses from
    one geostrophically balanced state to another
  • Geostrophic Balance PGF CF

6
QG OMEGA EQUATION (BASIC FORM)
  • (A) (B)
  • Regions of UPWARD MOTION
  • ? Vorticity Advection increasing w/height (A)
    WAA (B).
  • Regions of DOWNWARD MOTION
  • ? Vorticity Advection decreasing w/height (A)
    CAA (B).

7
FORMS OF OMEGA EQUATION
  • BASIC QUASIGEOSTROPHIC
  • Q-VECTOR
  • TRENBERTH
  • (2) AND (3) ACCOUNTS FOR CANCELLATION FEATURE
    FOUND IN (1).
  • APPROXIMATE TRENBERTH
  • NEGLECTS DEFORMATION TERM
  • EXTENDED
  • INCLUDES AGEOSTROPHIC WIND

8
  • Surface/Upper-Air Data 0000 UTC Nov. 2nd to 0000
    UTC Nov. 3rd
  • 2-pass Barnes Analysis Scheme
  • 25x17 grid
  • Dashed Box Computational Domain
  • Solid Box
  • Display Domain

9
Comparison Methods
  • LAYER EXAMINED 700-300mb AVERAGED VERTICAL
    MOTIONS
  • CORRELATIONS/ MEAN ABSOLUTE VALUES
  • SYNOPTIC PATTERNS
  • OMEGA vs. SYNOPTIC FEATURES
  • PRECIPITATION PATTERNS
  • PRECIP IN UPWARD MOTION

10
12 UTC 2 Nov. 1999 (TOP)SL Pressure
6hr. Precip. (MIDDLE)500-mb Height Abs.
Vort. (BOTTOM) 200-mb Height Winds
984 mb 0000 3rd
1000 mb 1200 2nd
1009 mb 0000 2nd
11
  • CC (omega patterns)
  • ?QG ?Q ?T ?AT
  • ?E 0.66 0.59 0.59 0.62
  • ?QG 1.00 0.91 0.96 0.90
  • ?Q xxxxx 1.00 0.95 0.85
  • ?T xxxxx xxxxx 1.00 0.90
  • MAV (omega magnitudes)
  • ?QG ?Q ?T ?AT ?E
  • 0.69 0.90 0.75 0.94
    0.89

12

TREN
EXT
AT
QG
500MB Z SOLID 700-300MB OMEGA DASHED SHADED
UPWARD MOTION
Q
13
PRECIP IN UPWARD MOTION
  • ?E ?QG ?Q ?T ?AT
  • 93 87 97 91 82
  • All results are similar in magnitude
  • No clear evidence of one form being superior

14
CONCLUSIONS
  • ALL VERTICAL MOTION FIELDS COMPARE FAVORABLY
    WITH SYNOPTIC FEATURES AND PRECIPITATION FIELDS.
  • CANNOT DETERMINE SUPERIOR METHOD USING SIMPLE
    SYNOPTIC AND PRECIPITATION COMPARISONS.
  • QG APPROXIMATION WORKS QUITE WELL EVEN FOR A CASE
    OF EXPLOSIVE CYCLONE DEVELOPMENT.
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