Versions Compared

Key

  • This line was added.
  • This line was removed.
  • Formatting was changed.

...

Section
Column

Lothar storm

Introduction

The Lothar storm that swept across Europe during 24-27 December 1999 is provided as a sample case study to use with OpenIFS. This storm was one of several severe storms to hit Europe in December 1999 and Lothar severely affected northern France, Switzerland and Germany (for more details see: Ulbrich et al., 2001, Weather, 56, 70-80).

The storms were characterized by record-breaking windspeed observations and rapid development across Europe. There was also a band of extremely high baroclinity near the cyclone track over the N. Atlantic and partly into Europe associated with Lothar.

The ECMWF forecasting system of the time did not accurately capture the storm's intensity though the strong jet stream was predicted some 9 days earlier. The storm initiated from a small disturbance in the Atlantic. More recently, Wedi et al, 2012, ECMWF Newsletter, have shown that very high resolution (T7999; ~2.5km) is necessary to accurately model accurately the high wind speeds observed, particularly over the mountainous regions of Europe.

A number of initial conditions are provided along with suggested exercises. Feedback on this case study (and others) is welcomed.

Column
width250px

 

 

Panel
bgColorwhite
titleBGColor#dcf0f7
titleOn this page...
borderStyledotted

Table of Contents
maxLevel3
indent10px

...

The ERA-Interim analysis is an improvement over the original analysis which did not have as many observations. The scientific content of the IFS operational model at that time was significantly different to the more modern OpenIFS. A rough proxy for the for  how the forecast at the time performed would be to run OpenIFS at T255, the resolution of the initial data.

Info

As OpenIFS is a spectral model, the 'T' number refers to the triangular truncation is in spectral space. Equivalent grid -pt resolutions are:
T159 is approximately ~ 125km resolution, T255 - ~ 80km, T511 - ~ 40km, T799 - ~ 25km, T1279 - ~ 16km.

Panel
borderColorgray
bgColorwhite
titleBGColor#e0e0e0
titleSingle start dates
borderStyledotted
Section
Column
width75%
ResolutionExpt idStart dateAnalysisFilenameFile size
T159L60fqar1999/12/24/12zERA-InterimT159_1999122412_fqar.tgz22Mb
T255L60fqak1999/12/24/12zERA-InterimT255_1999122412_fqak.tgz54Mb
T511L60fqaj1999/12/24/12zERA-InterimT511_1999122412_fqaj.tgz205Mb
T1023L60fs2y1999/12/24/12zERA-InterimT1023_1999122412_fs2y.tgz780Mb
T1279L60fqaf1999/12/24/12zERA-InterimT1279_1999122412_fqaf.tgz1.2Gb
Column
Info

To unpack files with .tgz, either use:

tar zxf T159_1999122412_fqar.tgz

or if your tar command does not support compression:

mv T159_1999122412_fqar.tgz T159_1999122412_fqar.tar.gz
gunzip T159_1999122412_fqar.tar.gz
tar xf T159_1999122412_fqar.tar

Panel
bgColorwhite
titleBGColor#e0e0e0
titleMultiple start dates
borderStyledotted
Section
Column
width70%
ResolutionExp idStart datesAnalysisFilenameFile size
T255g8oz1999/12, 14th-25th, 12zERA-InterimT255_199912_14-25_g8oz.tar.bz2660Mb
T511g8su1999/12, 14th-25th, 12zERA-InterimT511_199912_14-25_g8su.tar.bz2 22.3Gb
T1279g8t31999/12, 14th-25th, 12zERA-InterimT1279_199912_14-19_g8t3.tar.bz2
T1279_199912_20-25_g8t3.tar.bz2
6Gb
Column
Info

These files use the 'bzip2' command rather than 'gzip', to achieve a better compression.

Uncompressing may take a long time depending on your system.

To uncompress:

bzip2 -d T255_199912_14-25_g8oz.tar.bz2
tar xf T255_199912_14-25_g8oz.tar

...

The 'ecmwf' directory contains the files as used produced at ECMWF to run when this experiment was run:

  • namelistfc : copy this file to 'fort.4' to run the experiment (modify as required)
  • NODE.001_01 : this is the model output file as run at ECMWF. If your run fails, it may be useful to compare with this file.

...

As ERA-Interim is an improved analysis, forecasts from these starting initial conditions will not reproduce the operational forecast of the storm as it was in 1999. Because of changes to the forecasting system, this is impossible to do reproduce with OpenIFS. A proxy is to run the model at the same resolution as the ERA-Interim data (T255) as this is close to the resolution of the operational model of the time. 

...

  • What's the impact of the different 'lead times' on the forecast of the storm (i.e. starting from different dates)?

  • What's the impact of resolution on the forecast of the storm: both for it's development and impact over areas worse hit in Europe?

  • Reduce the timestep of the model - does this improve or worsen the forecast?

  • Reduce the gravity wave drag - how does this affect the forecast in the upper and lower levels?

    Expand
    titleHow to change the code (click here to expand)

     Edit the source code to half the gravity wave drag coefficient

    File: ifs/phys_ec/sugwd.F90, change:

    Code Block
    Line 108: !  Revised gwd parameter values
    Line 109: GKDRAG =0.15_JPRB

    to:

    Code Block
    Line 108: !  Revised gwd parameter values
    Line 109: GKDRAG = 0.075_JPRB   !  half GWD coefficient: 0.15_JPRB
  • Increase the precipitation auto conversion rate - what impact does this have?

    Expand
    titleHow to change the code (click here to expand…)

    Edit the source code to increase the auto conversion rate by 20%

    File: ifs/phys_ec/sucldp.F90, change:

    Code Block
    line 123: RKCONV=1._JPRB/6000._JPRB   ! 1/autoconversion time scale (s)

    to:

    Code Block
    line 123: ! RKCONV=1._JPRB/6000._JPRB   ! 1/autoconversion time scale (s)
    line 124: RKCONV=1.2_JPRB/6000._JPRB    ! default scaled by 20%: 1/autoconversion time scale (s)
  • Change the surface transfer coefficient in the turbulence scheme

    Expand
    titleHow to change the model code (click here to expand)

    Reduce the coefficient by 20%.

    Alter surf/module/surfexcdriver_ctl_mod.F90 from :

    Code Block
    line 671:  DO JL=KIDIA,KFDIA
    line 672:    IF (JTILE == IFRMAX(JL)) THEN 
    line 673:      PKHLEV(JL)=ZKHLEV(JL)
    line 674:    ENDIF
    line 675:  ENDDO

    to:

    Code Block
    line 671:  DO JL=KIDIA,KFDIA
    line 672:    IF (JTILE == IFRMAX(JL)) THEN 
    line 673:      PKHLEV(JL)=ZKHLEV(JL)
    line 674:    ENDIF
    line 675:    !  reduce surface transfer coeff by 20% in turbulence scheme
    line 676:    ZCFMTI(JL,JTILE)=0.8_JPRB*ZCFMTI(JL,JTILE)
    line 677:  ENDDO
  • Reduce (halve) the asymptotic mixing length scale (K)

    Expand
    titleHow to change the model code (click here to expand)

    For this change, two files need to be edited:

    Code Block
    titleifs/phys_ec/suvdf.F90
     line 53: RLAM   = 75.0_jprb  !! 150._JPRB: reduce to 75m 

    and:

    Code Block
    titleifs/phys_ec/vdfexcu.F90
     ZKLEN     = 75.0_jprb  !! 150.0_JPRB     ! asymptotic K length scale troposphere - Reduce to 75m
  • For these last 4 cases where the model's parametrizations have been altered, which make the biggest difference and why? Does any of the changes improve the forecast in any way?

  • If you were providing forecasts for wind and precipitation to the general public based on these experiments, what could you say with certainty and what is less certain? How would this change over different countries?

 

 

Further reading

Ulbrich et al., 2001, Weather, 56, 70-80

...