Proceedings - C-SRNWP Project
Proceedings - C-SRNWP Project
Proceedings - C-SRNWP Project
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scaling factor α and of the latent heat nudging temperature increments often occur. To<br />
mitigate this, the upper limit for α is reduced to 2 and the lower limit increased accordingly to<br />
0.5. Furthermore, the linear scaling is replaced by a logarithmic scaling, leading to effective<br />
limits of 1.7 and 0.3, respectively. This adaptation reduces the simulated precipitation<br />
amounts during the LHN.<br />
• In downdraft regions further upstream in convective cells, high precipitation rates occur<br />
often where latent heating is weak or even negative in most vertical layers. In order to avoid<br />
negative LHN temperature increments and cooling where the precipitation rate should be<br />
increased (and vice versa), only the vertical model layers with positive simulated latent<br />
heating are used to compute and insert the LHN increments. This modification tends to render<br />
the increments more coherent and the scheme more efficient.<br />
• Precipitation produced by the prognostic scheme will take some time to reach the ground<br />
where it is compared to the radar-derived surface precipitation rate. Thus, the conventional<br />
LHN scheme can notice only with some temporal delay when it has already initiated<br />
precipitation aloft. Therefore, a more immediate information on the precipitation rate already<br />
initialised is required, i.e. a sort of undelayed 'reference precipitation' which is used merely to<br />
replace the delayed prognostic model precipitation in the computation of the scaling factor α.<br />
One choice to work reasonably well is found to be the vertically averaged precipitation flux.<br />
a) b)<br />
Figure 1. Mean equitable threat score (a) and mean frequency bias (b) for hourly precipitation (threshold 0.1 mm) for the<br />
overall (combined 0 and 12 UTC forecast) runs as a function of forecast time. The thin vertical purple lines indicate the<br />
starting time of the free forecasts. The “mean” scores were obtained by adding up the contingency table over a 45-day period.<br />
Assimilation cycles: nudging without LHN (blue dashed, label “LMK TS 2.6 (5784)”) and nudging with LHN (green solid,<br />
label “LMK TS 3.3b (5730)”). The red bars at the bottom of the panels show the number of observed precipitation events<br />
above the considered threshold value.<br />
3. VERIFICATION OF MODELLED AGAINST RADAR-OBSERVED<br />
PRECIPITATION<br />
For an assessment of the overall performance of the revised LHN during assimilation and<br />
especially for an evaluation of LHN's forecast impact, two experiments using the COSMO<br />
model in the 2.8km version (LM-K) of the German weather service (DWD) have been carried<br />
out for a 45-day period in June and July 2006. A LHN experiment, comprising of an LM-K<br />
assimilation run with LHN and two daily 24-hour forecasts starting at 0 and 12 UTC, is<br />
compared to a control experiment, which has been set up in the same way but does not use<br />
LHN during assimilation. The particular comparison measures are “Equitable Threat Score”<br />
(ETS) and “Frequency Bias” (FBI) for hourly precipitation.<br />
On average, the positive impact of radar data is visible in the combined 0 and 12 UTC<br />
forecasts’ ETS for up to 5 hours for a threshold value of 0.1 mm (fig. 1a). This impact time<br />
decreases slightly for higher threshold values (not shown). Whether the rapid decrease of ETS<br />
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