Three-dimensional modeling of synthetic cold fronts interacting with northern Alpine foehn |
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Authors: | Dr. D. Heimann |
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Affiliation: | (1) Present address: Institut für Physik der Atmosphäre Obserpfaffenhofen, Deutsche Forschungsanstalt für Luft-und Raumfahrt, Weßling, D-W-8031, Germany |
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Abstract: | Summary The effect of the Alpine orography on prototype cold fronts approaching from the west is investigated by three-dimensional numerical model simulations. The numerical experiments cover a range of parameter constellations which govern the prefrontal environment of the front. Especially, the appearance and intensity of prefrontal northern Alpine foehn varies from case to case.The behaviour of a cold front north of the Alps depends much on the prefrontal condition it encounters. It is found that prefrontal foehn can either accelerate or retard the approaching front.An important feature is the pressure depression along the northern Alpine rim that results from the southerly foehn flow. In cases where this depression compensates the eastward directed pressure gradient associated with the largescale flow, the front tends to accelerate and the foehn breaks down as soon as the front passes. In contrast, the foehn prevents the front from a rapid eastward propagation if it is connected with a strong southerly wind component.No-foehn experiments are performed for comparison, where either the mountains are removed, or the static stability is set to neutral. Also shown are effects of different crossfrontal temperature contrasts.List of Symbols cF propagation speed of a front - x, y horizontal grid spacing (cartesian system) - , horizontal grid spacing (geographic system) - t time step - z vertical grid spacing (cartesian system) - cross-frontal potential temperature difference - i potential temperature step at an inversion - E turbulent kinetic energy - f Coriolis parameter - FGP frontogenesis parameter (see section 2.2) - g gravity acceleration (g=9.81 m s–2) - vertical gradient of potential temperature - h terrain elevation (above MSL) - hi height of an inversion (hi=1000 m MSL) - H height of model lid (H=9000 m MSL) - KM exchange coefficient of momentum - KH exchange coefficient of heat and moisture - longitude - N Brunt-Väisäla-frequency - p pressure - Exner function (=T/) - latitude - qv specific humidity - Rd gas constant of dry air (Rd=287.06 J kg–1 K–1) - density of dry air - t time - T temperature - potential temperature - TFP thermal front parameter (see section 2.2) - u, v, w cartesian wind components - ug,vg geostrophic wind components - horizontal wind vector - x, y, z cartesian coordinatesAbbreviations GND (above) ground level - MSL (above) mean sea level - UTC universal time coordinatedWith 20 Figures |
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