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46<br />
this season, as well as the higher residency time (Picher et<br />
al. 2008) that could provide a longer time for small-scale<br />
features spin-up.<br />
to be attributable to the fact that the different large-scale<br />
circulation occurring in L1W does not allow such feature<br />
to develop.<br />
Figure 1. Small-scale transient eddies of the 700-hPa<br />
relative humidity for a) BW, b) BS, c) L4W and d) L4S. The<br />
scale is given in %. The spatial correlation coefficient (R*)<br />
with BW and BS for L4W and L4S are of 50 and 90%<br />
respectively.<br />
4. Effect of spectral nudging at large scales<br />
This section focuses on how applying SN can affects<br />
development of small-scale features simultaneously with<br />
variations of the domain size. On Fig. 2 are shown the smallscale<br />
transient eddies of the 700-hPa relative vorticity for the<br />
virtual reference simulation (BW; Fig. 2 a), the largedomain<br />
Little-Brother using SN (L1WN; Fig. 2 b) and<br />
without SN (L1W; Fig. 2 c) and a smaller domain Little-<br />
Brother with no SN (L3W; Fig. 2 d). See Tab. 1 for an<br />
overview of simulations.<br />
Let’s first concentrate on the similarities between patterns<br />
by using the spatial correlation coefficient of the Little-<br />
Brothers with the virtual reference climate (BW). L1W<br />
displays the most different pattern with R* = 50% compared<br />
to 79 and 72% for L1WN and L3W respectively. Since<br />
small-scales features are somewhat preconditioned by the<br />
large-scale information penetrating the domain through its<br />
lateral boundaries, the fact that L1W shows such a different<br />
small-scale pattern is principally attributable to the use of a<br />
large domain without applying SN. Such conditions<br />
engender a weak control of the LBC on the RCM large-scale<br />
solution, and have a consequence on the small-scale<br />
features. For the cases of L1WN and L3W, skills for pattern<br />
matching with BW are higher than L1W for two different<br />
reasons. L1WN uses a strong SN allowing a sufficient<br />
control of the nesting data on the large-scale solution, in<br />
despite of its large domain. Also, the large domain allows<br />
for a sufficient distance needed to spin-up the small-scale<br />
transient eddies. For L3W, SN does not seem required to<br />
obtain a significant matching in small-scale feature patterns<br />
since proximity of the lateral boundaries from the validation<br />
area provides the control needed for keeping the large-scale<br />
flow similar to the driving data.<br />
Another interesting point is about potential side effects that<br />
may be related to the use of a strong SN (Alexandru et al.<br />
2009). From the results presented on Fig. 2, effect of SN on<br />
intensity of small-scale transient eddies is not significant<br />
when averaged overall the domain. However, it is clearly<br />
visible that the southern maximum is not captured by the<br />
large-domain simulation without SN (Fig. 2 c). This seems<br />
Figure 2. Small-scale transient eddies of the 700-hPa<br />
relative vorticity for a) BW, b) L1WN, c) L1W and d)<br />
L3W. The scale is given in 1.0e-05 s -1 . The spatial<br />
correlation coefficient (R*) with BW for L1WN, L1W and<br />
L3W gives respective values of 79, 50 and 72 %.<br />
5. Conclusions<br />
The domain-size perfect-model experiment for a winter<br />
short climate (LL08) has been compared with new results<br />
obtained for the summer season. Simulations presented<br />
here display a seasonal dependence of the domain-size<br />
effect on the small-scale transient eddies. For winter, a<br />
small domain of integration engender lacks in the transient<br />
variability of the small-scale features, particularly on the<br />
inflow side of the domain. In summer, simulations also<br />
display such underestimations but those are homogenously<br />
distributed overall the domain of interest. Differences in<br />
the ventilation regimes that depend on season seem to<br />
partly explain such different spatial spin-up. By<br />
performing supplementary winter experiments using a<br />
strong SN permitted a direct comparison of the smallscales<br />
features for different domain sizes since the largescale<br />
flow remains approximately the same. By this way,<br />
it has been possible to isolate the effect of the distance<br />
traveled by the inflow to explain the differences residing<br />
in the intensity of small-scales transient eddies.<br />
References<br />
Alexandru, A., R. de Elia, R. Laprise, L. Separovic and S.<br />
Biner, 2009: Sensitivity Study of Regional Climate<br />
Model Simulations to Large-Scale Nudging<br />
Parameters. Mon. Wea. Rev. (accepted)<br />
de Elía R, Laprise R, Denis B, 2006: Forecasting skill<br />
limits of nested, limited-area models: a perfect-model<br />
approach. Mon. Wea. Rev., 130:2006–2023<br />
Leduc, M. and R. Laprise, 2008: Regional Climate Model<br />
sensitivity to domain size. Clim. Dyn., (Published<br />
online, DOI 10.1007/s00382-008-0400-z).<br />
Lucas-Picher, P., D. Caya, S. Biner and R. Laprise, 2008:<br />
Investigation of regional climate models’ internal<br />
variability with a ten-member ensemble of 10-year<br />
simulations over a large domain. Mon. Wea. Rev.,<br />
136:4980-4996.