numerial simulations of convective events – the effect of propagating gust fronts

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Numerial Simulations of Convective Events The Effect of Propagating Gust Fronts Kaspar and Müller ([email protected]) Institute of Atmospheric Physics ASCR, Prague, CR

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Numerial Simulations of Convective Events – The Effect of Propagating Gust Fronts. Kaspar and Müller ([email protected]) Institute of Atmospheric Physics ASCR, Prague, CR. H – head height. Simpson (1972). H. gust front. Motivation. - PowerPoint PPT Presentation

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Page 1: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

Numerial Simulations of Convective Events

– The Effect of Propagating Gust Fronts

Kaspar and Müller ([email protected])

Institute of Atmospheric Physics ASCR, Prague, CR

Page 2: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

- collision with other gust fronts and convergence lines (Wilson and Schreiber, 1986)

Interaction with environmental air – convection initiation - interaction with ambient vertical shear

(Thorpe et al., 1980; Rotunno, 1988; Moncrieff and Liu, 1999) - interaction with mesoscale oscillations

(Crook et al., 1990)

Gust front = an advancing surface boundary of the outflow of thunderstorm downdrafts cooled by evaporation.

Nowcasting, numerical and analytical studies.(Droegemeier and Wilhelmson, 1987; Liu and Moncrieff, 1996b)

H

H – head heightSimpson (1972)

gust front

Motivation

Page 3: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

Methodology (Kaspar, 2003)

LM COSMO thermodynamic data, 2.8km (Doms and Schättler, 1999)

Model for the Objective Analysis of Gust Fronts (OAGF)

LOCATION 3-dim. position (thermal def.)

head heightMORPHOLOGY

MOVEMENT speed vector

VERTICAL SHEAR regime of propagation (Liu and Moncrieff, 1996a)

STABILITY potential instability, LCL

Page 4: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

Propagating regimeUpshear movementDownshear movement

Steering-level (hs) regimeDownshear movement with an overturning updraft

Vertical shear conditions

Relative flow1

2

3

1

2

3

Convection initiation(a) PI and a low LCL

all regimes(b) PS and / or a high LCL

the steering-level and downshear prop. regime

Page 5: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

OA gust fronts + surface precipitation rates [mm/h]OA gust fronts + vertical velocities [m/s]OA gust fronts + potential temperature [K]

Case study 2.7.2000- validation tests

Radar SkalkyZmax

13UTC 14UTC 15UTC

Page 6: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

Case study 2.7.2000Height of OA gust heads + RSM [dBZ] (Haase and Crewell, 2000)

Downshear propagating regime

c0=7.1m/sH =1180m

PI + decreasing LCL

Page 7: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

Case study 22/23.7.1998- squall line (Salek, 2000)

01UTC 02UTC 03UTC

SkalkyZmax

OA gust fronts + surface precipitation rates [mm/h]

Page 8: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

Case study 22/23.7.1998OA gust heads + RSM [dBZ]

Steering-level regime

c0=5.1m/sH=1343m

Potential stability + increasing LCL

Page 9: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

Conclusions

The validation tests confirmed the applicability of the LM COSMO-OAGF chain in the case of both isolated and multicellular convection.

The propagating gust fronts had the potential for convection initiation in both presented case studies.- 2 July 2000:

favourable vertical shear, humidity and stability conditions- 22 / 23 July 1998:

favourable vertical shear conditions

- the both case studies are included in a paper accepted for Atmospheric Research (2006)

Page 10: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

The tuning and verification of the OAGF will continue.- radar data assimilation- locating procedures based on the analysis of wind field …

The products of the OAGF are assumed to be used in formulating decision criteria.- total index quantifying the potential of a gust front to trigger

new convection

Outlooks

Acknowledgement: GA ASCR B3042404, GACR 205/04/0114DWD (LM and RSM codes), CHMI (radar pictures)

Page 11: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

thank you for your attention

Page 12: Numerial Simulations  of Convective Events –  The Effect of Propagating  Gust Fronts

References:Crook, N.A., Carbone, R.E., Moncrieff, M.W., Conway, J.W., 1990. The generation and propagation

of a nocturnal squall line. Part II: Numerical simulations. Mon. Weather Rev. 118, 50-65.Doms, G., Schättler, U., 1999. The Nonhydrostatic Limited-Area Model LM of DWD. Part I: Scientific

Documentation, DWD, Offenbach, Germany, 172 pp., available at http://www.cosmo-model.org.Droegemeier, K.K., Wilhelmson, R.B., 1987. Numerical simulation of thunderstorm outflow dynamics.

Part I: Outflow sensitivity experiments and turbulence dynamics. J. Atmos. Sci. 44, 1180-1210. Haase, G., Crewell, S., 2000. Simulation of radar reflectivities using a mesoscale weather forecast

model. Water Resources Research 36, 2221-2231. Hewson T.D., 1998. Objective fronts. Meteorol. Appl. 5, 37-65.Kaspar, M., 2003. Analyses of gust fronts by means of limited area NWP model outputs. Atmos. Res.

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Sci. 45, 463-485. Salek, M., 2000. Torrential rainfalls in the foothills of the Orlicke hory Mts. on the 22 and 23 July 1998

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Simpson, J.E., 1972. Effects of the lower boundary on the head of a gravity current. J. Fluid Mechs. 53, 759-768.

Thorpe, A. J., Miller, M.J., Moncrieff, M.W., 1980. Dynamical models of two-dimensional downdraughts. Q. J. R. Meteorol. Soc. 106, 463-484.

Wilson, J. W., Schreiber, W.E., 1986. Initiation of convective storms at radar-observed boundary-layer convergence lines. Mon. Wea. Rev. 114, 2516-2536.