SIMULATION OF MAP CASE 1: Vaison-la-Romaine

MAP EPISODE

 Vaison-la-Romaine Flash Flood , 20-24 septembre 1992.

TIME WINDOW

Run 50km: 920921 00UTC to 920923 12UTC
Run 10km: 920921 06UTC to 920923 12UTC

MODEL USED

MC2 v3.4.3 (Benoit et al, 1997)

PROVIDER

Robert BENOIT
Recherche en Prevision Numerique, Dorval, Canada
Robert.Benoit@ec.gc.ca

SIMULATION DOMAINS

NW NE SW SE
50km 54.37N 
61.38W
54.29N 
81.42E
18.99N 
15.27W
18.96N 
35.33E
10km 53.10N 
15.61W
55.70N 
22.84E
33.83N 
05.68W
35.21N 
17.61E
Geographic projection: Polar Stereographic true at 60 degrees north
Domain and Orography : 50km - 10km
Orography data : GLOBE dataset for the 10, US NAvy for the 50km domain
All 2 domains, 50km orography and simulation time window information.

COMPUTATIONAL GRID

Model Lid (rigid lid): 25 000 m (rigid top boundary condition)
Vertical Coordinate:  Gal-Chen 
Z(X,Y,z) = H * [z - h(X,Y)] / [H - h(X,Y)] 
Z : Gal-Chen Height 
z : Physical Height 
H : model lid 
h : model topography
 
 
NI (x) NJ (y) NK (z)
50km  147 131 29 (list)
10km  254  254  35 (list)

INITIAL AND NESTING FIELDS

50 km Run:  ECMWF Uninitialized Analysis 
(directly in terrain following coordinate)
10 km Run:  Model is self-nested in the 50 km Run 

ACTIVATED PHYSICAL PARAMETERIZATION

Common to all resolutions:
Specific to each resolution:
 
50km 10km
Large scale precip. Kessler  Kessler 
Convective precip. Kuo  FCP 
Gavity wave drag 
(McFarlane 1987)
yes  yes 
Horizontal Diffusion 
Coefficient KH [m2/s]
25000. 3000.
Kessler : Explicit cloud and rain water prediction based on Kessler (1969)
Kong & Yau: Microphysic Scheme described in Kong and Yau 1996 (Atmos.-Ocean, May 1996)
Kuo: Kuo Convection Scheme (Kuo 1974) similar to the version used at ECMWF (1984)
FCP : Fritsch-Chappell scheme (1980) as modified by Zhang and Fritsch (1986)

AVAILABLE FIELDS

The diagnostic quantities HR (Relative humidity), PV (Potential vorticity) and TH (Potential temperature) are computed with home made routines and so is GZ (Geopotential Height).
The graphics are made using the displaying tool GI_MAP available at MDC.
The symbols used in the table are as follow:
 
PR: Total Precipitation Accumulation (3h or 24h, the date mark the beginning of the period) [mm]
SN: Convective Precipitation Accumulation (3h or 24h, the date mark the beginning of the period) [mm]
PN: Mean Sea Level Pressure [hPa]
GZ: Geopotential Height [dm]
UV: Wind, Horizontal Component [m/s]
WZ: Wind, Vertical Component [m/s]
TH: Potential Temperature [K]
HR: Relative Humidity [%]
PV: Potential Vorticity [PVU]
For further information please contact Robert Benoit or Stephane Chamberland.

REM: The 50km figures are not available. Info about this run have been included as a reference for the self nesting procedure.

List of available field :
 

Run Field Level Dates
10km PR3, SN3 Surface 092192 06 UTC to 092392 09 UTC (every 3h)
PR24h, SN24 Surface 092192 06 UTC and 092292 06 UTC
PN, UV Surface 092192 06 UTC to 092392 12 UTC (every 3h)
GZ, UV, WZ, 
TH, HR
300 mb 
500 mb 
850 mb
092192 06 UTC to 092392 12 UTC (every 3h)
PV 850 mb 
310 K 
315 K
092192 06 UTC to 092392 12 UTC (every 3h)
  Download hi-resolution figures:

 

Surface 850 mb 500 mb 300 mb 310 K 315 K
PR 520 Kb          
SN 493 Kb          
PN 1547 Kb          
GZ   462 Kb 491 Kb 466 Kb    
UV 994 Kb 935 Kb 819 Kb 920 Kb    
WZ   886 Kb 805 Kb 751 Kb    
TH   534 Kb 471 Kb 462 Kb    
HR   992 Kb 747 Kb 683 Kb    
PV   977 Kb     783 Kb 858 Kb
table entries indicate the file size
 
Look at  low resolution figures:
(Use SAVE IMAGE AS option to download the image)

To change the figure above, select relevant options then press the corresponding show button.
Type of field:
Level:
10 km:
How to read the informations on the figure

REFERENCES

Benoit, R., J. Cote and J. Mailhot, 1989: Inclusion of a TKE boundary layer parameterization in the Canadian regional finit-element model. Mon. Wea. Rev., 117, 1726-1750.

Benoit, R., M. Desgagne, P. Pellerin, S. Pellerin, Y. Chartier and S. Desjardins, 1997: The canadian MC2: A semi-lagrangian, semi-implicit wide-band atmospheric model suited for fine-scale process studies and simulation. Mon. Wea. Rev., Vol 125 (in press).

Deardorff, J.W., 1976: Efficient prediction of grounds surface temperature and moisture with inclusion of a layer of vegetation. J.Geophy. Res., 83, 1889-1903.

Fouquart, Y. and B. Bonnel, 1980: Computation of solar heating of the eart's atmosphere: a new parameterisation. Contrib. Atmos. Phys., 53, 35-63.

Garand, L., 1983: Some improvement and comlements of the infrared emissivity algorithm including a parameterization of the absorption in the continuum region. J. Atmos. Sci., 40, 230-244.

Garand, L. and J. Mailhot, 1990: The influence of the infrared radiation on numerical weather forecasts. Proceedings of the Seventh Conference on Atmospheric Radiation, 23-27 July 1990, San Francisco, U.S.A., Amer. Meteor. Soc., J146-J151.

Georgelin, M., E. Richard, M. Petitdidier and A. Druilhet, 1994: Impact of subgrid-scale orography parameterization on the simulation of orographic flows. Mon. Wea. Rev., 122, 1509-1522.

Kessler, E., 1969: On the distribution and continuity of water substance in atmospheric circulation. Meteor. Monogr., 10, No. 32, Amer. Meteor. Soc., 84 pp.

Kong F. and K. Yau, 1997: An Explicit Approach of Microphysics in MC2. Submitted to Atmos.-Ocean.

Kuo, H. L., 1974: Further studies on the parameterization of the influence of cumulus convection on large-scale flow. J. Atmos. Sci., 31, 1232-1240.

McFarlane, N.A., 1987: The efect of orographically excited gravity wave drag on the general circulation of the lower stratosphere and troposphere. J. Atmos. Sci., 44, 1775-1800.