Title: Propagation of a Front, Encountering a Cold Air Layer
1Propagation of a Front, Encountering a Cold Air
Layer
- Jeroen Derksen
- u.s.o. Aarnout van Delden
2Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
3Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
4Introduction
- Typical setting over western Europe during
winter. - Cold air over Land.
- Relatively warm Sea.
- Decreasing propagation of a front
- Hard to forecast.
- Arrival of warm air forecasted to early
- Stalling front over cold air
- snow, sleet
- Hazardous weather.
5Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
6Case Study
- 5 and 6 January 1995
- Satellite Infrared Photos
- ECMWF-data
- Height and Temperature of 1000hPa surface
- Equivalent Potential temperature
- Cross-section over the Netherlands
7Case Study
Infrared Satellite Pictures
0903UTC 5 Jan
1942UTC 5 Jan
0936UTC 6 Jan
8Case Study II
Isotherms and Height 1000hPa Sfc.
00UTC 5 Jan
9Case Study III
Equivalent Potential Temperature 700hPa Sfc.
12UTC 5 Jan.
10Case Study IV
Equivalent Potential Temperature 700hPa Sfc.
00UTC 6 Jan.
11Case Study VI
Equivalent Potential Temperature 700hPa Sfc.
12UTC 5th
00UTC 5th
00UTC 6th
12UTC 6th
12Case Study VII
Cross-section 52N, 5 Jan
00UTC
12UTC
13Case Study VIII
Cross-section 52N, 6 Jan
00UTC
12UTC
14Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
15Basic Equations
- Full set of Equations are not solvable
- Range of approximated sets developed.
- Geostrophic Balans
- Geostrophic momentum approximation
16Geostrophic Balans
- Geostrophic Balans.
- Hydrostatic Balans
- Thermal Wind Balans
17Thermal Wind Balance
- Difference in sign.
- Geostrophic disturbance leads away from thermal
wind balance. - Ageostrophic motion needed.
18Geostrophic Momentum Approximation
19Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
20Frontogenesis
- Geostrophic
- confluence of temperature field due to
geostrophic wind field - rotation of isentropes due to geostrophic shear
- Ageostrophic
- tilt of vertical temperature gradient onto
horizontal due to horizontal gradient in vertical
velocity - differential diabatic heating
21Frontogenesis II
22Frontogenesis III
23Frontogenesis IV
24Frontogenesis V
25Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
26Sawyer-Eliassen Eqn.
- Cross-frontal Circulation
- Based on Geostrophic Momentum Approximation.
- Assumptions
- Straight Front
- 2 Dimensional Front
- Coriolis Parameter Constant
27System
- 2D
- Straight
- Cross-frontal circulation.
28Sawyer-Eliassen Eqn. II
- ? Streamfunction
- a Measure of Static Stability
- b Cross-Frontal Temperature Gradient
- c Geostrophic Absolute Vorticity
- F Geostrophic Forcing
29Examples
Reference Circulation
30Examples II
Sign forcing changed
31Examples III
a smaller
32Examples IV
c larger
33Examples V
Neg.
Pos.
b larger
34Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
35Model
- No Differential Diabatic heating
- No North-South Temperature Gradient
36Model II
- All the variables are obtained, using ECMWF-data,
except for y.
37Model III
- Solving S-E, using the Relaxation Scheme.
- Guessed Solution -gt Residu
- Residu -gt Next Solution
- etc.
- -gt Right Solution
38Model IV
- Guessed solution on iteration step m
- Suppose next iteration step, m1, gives correct
answer, using the old values of ? on step m on
the surrounding gridpoints
39Model V
40Model VI
Boundary conditions
- Bottom ? 0.
- Both sides vertically integrated ua,, obtained
from ECMWF-data. - Top
- Difference both sides
- Continuity
- Difference spread over top
41Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
42Result
- Sawyer-Eliassen Equation
- Forcing Geostrophic confluence
- Influence Boundaries?
- Larger Domain 19WL-29EL
43Result 00UTC 5 Jan
red calculated circulation green observed
ageostrophic circulation
44Result 06UTC 5 Jan
red calculated circulation green observed
ageostrophic circulation
45Result 12UTC 5 Jan
red calculated circulation green observed
ageostrophic circulation
46Result 18UTC 5 Jan
red calculated circulation green observed
ageostrophic circulation
47Result 00UTC 6 Jan
red calculated circulation green observed
ageostrophic circulation
48Contents
- Introdction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
49Discussion
- 5 January Results are good.
- 6 january Results are not good.
- Which of the neglected terms is responsible?
- Confluence by total wind field
- Shear-term
- Tilting-term
- Differential Diabatic Heating
50Discussion II
- Confluence by total wind field adds nothing new.
- Shear term stronger on the fifth than on the
sixth. - Tilting term to weak.
- Differential Diabatic heating?
51Discussion III
Diabatic heating
Differential Diab. Heating
52Discussion IV
Circulation, taking Diff. Diab. Heating into
account
06UTC 5 Jan.
red calculated circulation green observed
ageostrophic circulation
53Discussion V
Circulation, taking Diff. Diab. Heating into
account
18UTC 5 Jan.
red calculated circulation green observed
ageostrophic circulation
54Discussion VI
Circulation, taking Diff. Diab. Heating into
account
00UTC 6 Jan.
red calculated circulation green observed
ageostrophic circulation
55Discussion VII
Circulation, taking Diff. Diab. Heating into
account
06UTC 6 Jan.
red calculated circulation green observed
ageostrophic circulation
56Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
57Conclusion
- A circulation cell is present over the boundary
of the cold air. - It is present, partly due to
- confluence of the temperature field by the
geostrophic wind field - Differential Diabatic Heating
- This cell is responsible for an easterly wind at
the surface. - The advection of cold air by this wind physically
blocks the oncoming warm air.
58Contents
- Introduction
- Case Study
- Theory
- Basic Equations
- Frontogenesis
- Sawyer-Eliassen Equation
- Model
- Result
- Discussion
- Conclusions
- Recommendations
59Recommendations
- Use higher resolution, in time and space.
- Make a more general model
- Dont assume the front to be North-South.
- Dont assume the front to be straight.
- Use a 3D model.
- Beware that processes are easily recognized.
- Study more events.
60Any Questions?