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Proceedings - C-SRNWP Project

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• However inspection of T2m forecasts in deep valleys, like around Grenoble (see Figure 2),<br />

revealed that an interaction between the above-described best ‘dynamical’ choice for SLHD<br />

and the AROME physical package created spurious spots of too hot temperatures, these<br />

spots disappearing when almost all horizontal diffusion is removed (a testing solution<br />

without any operational application, of course).<br />

SLHD=T (daily run) :<br />

SLHD=F (& very small sp. diff.)<br />

Problem areas in SLHD run<br />

OK but not a solution (too<br />

noisy elsewhere)<br />

Figure 2: Illustration of the valley ‘hot-spots’ problem (on the left). It can be cured (on the<br />

right) by removing nearly all kind of lateral diffusion, spectral and/or SLHD, but this is not a<br />

viable solution for a full purpose NWP model. The solution (not shown but quasi identical to<br />

that of the picture on the right) will surprisingly come from a study about the intrinsic SLHD<br />

behaviour. Courtesy of Yann Seity.<br />

• Inspection of the spectral behaviour of SLHD, visualised through the vertical divergence<br />

(closely linked to the vertical velocity w) created a big surprise (see Figure 3). The studied<br />

syndrome was a ‘bifurcation-type’ one. Indeed the spectra with vanishing residual diffusion<br />

on w were radically differing from the whole effect, with the zero solution in between! Of<br />

course, this immediately lead to a solution without hardly any sign of either the ‘chimney<br />

syndrome’ or the presence of ‘hot-spots’, solution obtained with a division by 15 of the<br />

intensity of the SLHD action on w.<br />

26

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