A numerical single-layer shallow water model is used to elucidate the dynamics of these gap flows. The model resolves real topography of the Wipp valley region with a mesh size of 500 meters. Various simulations are performed with different initial upstream Froude-numbers (0.25 to 2) and layer heights (1.5 to 5 km MSL). In most cases, the flow becomes first critical near Brenner pass due to the vertical and lateral constriction of the gap. A few kilometers downstream, the associated jump occurs where the flow becomes subcritical again. However, the flow speeds up again due to the general subsidence of the layer surface. Observational data show highest near-surface wind speeds in the lower third of the Wipp valley, i.e. about 20 km north of Brenner. The model reproduces the location of this maximum together with a hydraulic jump further downstream. Flow transition near this region occurs only if the far downstream reservoir height is lower then the height upstream of the pass. In reality such a pre-existing difference in reservoir height is resembled by a synoptic pressure gradient and enhanced hydrostatically due to cold blocked air upstream of the pass.
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