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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.

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