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  • 1
    Online Resource
    Online Resource
    Wiley ; 2008
    In:  Quarterly Journal of the Royal Meteorological Society Vol. 134, No. 633 ( 2008-04), p. 817-839
    In: Quarterly Journal of the Royal Meteorological Society, Wiley, Vol. 134, No. 633 ( 2008-04), p. 817-839
    Type of Medium: Online Resource
    ISSN: 0035-9009 , 1477-870X
    URL: Issue
    RVK:
    RVK:
    Language: English
    Publisher: Wiley
    Publication Date: 2008
    detail.hit.zdb_id: 3142-2
    detail.hit.zdb_id: 2089168-4
    SSG: 14
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  • 2
    Online Resource
    Online Resource
    American Meteorological Society ; 2011
    In:  Journal of the Atmospheric Sciences Vol. 68, No. 9 ( 2011-09-01), p. 2107-2127
    In: Journal of the Atmospheric Sciences, American Meteorological Society, Vol. 68, No. 9 ( 2011-09-01), p. 2107-2127
    Abstract: Observations show that on a mountainside the boundary between snow and rain, the snow line, is often located at an elevation hundreds of meters below its elevation in the free air upwind. The processes responsible for this mesoscale lowering of the snow line are examined in semi-idealized simulations with a mesoscale numerical model and in simpler theoretical models. Spatial variations in latent cooling from melting precipitation, in adiabatic cooling from vertical motion, and in the melting distance of frozen hydrometeors are all shown to make important contributions. The magnitude of the snow line drop, and the relative importance of the responsible processes, depends on properties of the incoming flow and terrain geometry. Results suggest that the depression of the snow line increases with increasing temperature, a relationship that, if present in nature, could act to buffer mountain hydroclimates against the impacts of climate warming. The simulated melting distance, and hence the snow line, depends substantially on the choice of microphysical parameterization, pointing to an important source of uncertainty in simulations of mountain snowfall.
    Type of Medium: Online Resource
    ISSN: 0022-4928 , 1520-0469
    RVK:
    Language: English
    Publisher: American Meteorological Society
    Publication Date: 2011
    detail.hit.zdb_id: 218351-1
    detail.hit.zdb_id: 2025890-2
    SSG: 16,13
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  • 3
    Online Resource
    Online Resource
    American Meteorological Society ; 2007
    In:  Journal of Hydrometeorology Vol. 8, No. 5 ( 2007-10-01), p. 1068-1081
    In: Journal of Hydrometeorology, American Meteorological Society, Vol. 8, No. 5 ( 2007-10-01), p. 1068-1081
    Abstract: Persistent, 10-km-scale gradients in climatological precipitation tied to topography are documented with a finescale rain and snow gauge network in the Matheny Ridge area of the Olympic Mountains of Washington State. Precipitation totals are 50% higher on top of an ∼800-m-high ridge relative to valleys on either side, 10 km distant. Operational fifth-generation Pennsylvania State University–NCAR Mesoscale Model (MM5) runs on a 4-km grid produce similar precipitation patterns with enhanced precipitation over high topography for 6 water years. The performance of the MM5 is compared to the gauge data for 3 wet seasons and for 10 large precipitation events. The cumulative MM5 precipitation forecasts for all seasons and for the sum of all 10 large events compare well with the precipitation measured by the gauges, although some of the individual events are significantly over- or underforecast. This suggests that the MM5 is reproducing the precipitation climatology in the vicinity of the gauges, but that errors for individual events may arise due to inaccurate specification of the incident flow. A computationally simple model of orographic precipitation is shown to reproduce the major features of the event precipitation pattern on the windward side of the range. This simple model can be coupled to landscape evolution models to examine the impact of long-term spatial variability in precipitation on the evolution of topography over thousands to millions of years.
    Type of Medium: Online Resource
    ISSN: 1525-7541 , 1525-755X
    Language: English
    Publisher: American Meteorological Society
    Publication Date: 2007
    detail.hit.zdb_id: 2042176-X
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  • 4
    Online Resource
    Online Resource
    Wiley ; 2003
    In:  Quarterly Journal of the Royal Meteorological Society Vol. 129, No. 588 ( 2003-1-1), p. 693-713
    In: Quarterly Journal of the Royal Meteorological Society, Wiley, Vol. 129, No. 588 ( 2003-1-1), p. 693-713
    Type of Medium: Online Resource
    ISSN: 1477-870X , 0035-9009
    RVK:
    RVK:
    Language: Unknown
    Publisher: Wiley
    Publication Date: 2003
    detail.hit.zdb_id: 3142-2
    detail.hit.zdb_id: 2089168-4
    SSG: 14
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  • 5
    Online Resource
    Online Resource
    American Meteorological Society ; 2021
    In:  Journal of the Atmospheric Sciences Vol. 78, No. 1 ( 2021-01), p. 313-327
    In: Journal of the Atmospheric Sciences, American Meteorological Society, Vol. 78, No. 1 ( 2021-01), p. 313-327
    Abstract: The dynamics of a prototypical atmospheric bore are investigated through a series of two-dimensional numerical simulations and linear theory. These simulations demonstrate that the bore dynamics are inherently finite amplitude. Although the environment supports linear trapped waves, the supported waves propagate in roughly the opposite direction to that of the bore. Qualitative analysis of the Scorer parameter can therefore give misleading indications of the potential for wave trapping, and linear internal gravity wave dynamics do not govern the behavior of the bore. The presence of a layer of enhanced static stability below a deep layer of lower stability, as would be created by a nocturnal inversion, was not necessary for the development of a bore. The key environmental factor allowing bore propagation was the presence of a low-level jet directed opposite to the movement of the bore. Significant turbulence developed in the layer between the jet maximum and the surface, which reduced the low-level static stability behind the bore. Given the essential role of jets and thereby strong environmental wind shear, and given that idealized bores may persist in environments in which the static stability is constant with height, shallow-water dynamics do not appear to be quantitatively applicable to atmospheric bores propagating against low-level jets, although there are qualitative analogies.
    Type of Medium: Online Resource
    ISSN: 0022-4928 , 1520-0469
    RVK:
    Language: Unknown
    Publisher: American Meteorological Society
    Publication Date: 2021
    detail.hit.zdb_id: 218351-1
    detail.hit.zdb_id: 2025890-2
    SSG: 16,13
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  • 6
    Online Resource
    Online Resource
    Elsevier BV ; 1979
    In:  Atmospheric Environment (1967) Vol. 13, No. 7 ( 1979-1), p. 1021-1037
    In: Atmospheric Environment (1967), Elsevier BV, Vol. 13, No. 7 ( 1979-1), p. 1021-1037
    Type of Medium: Online Resource
    ISSN: 0004-6981
    Language: English
    Publisher: Elsevier BV
    Publication Date: 1979
    detail.hit.zdb_id: 216368-8
    detail.hit.zdb_id: 2140521-9
    detail.hit.zdb_id: 1499889-0
    detail.hit.zdb_id: 1017027-3
    SSG: 13
    SSG: 14
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  • 7
    Online Resource
    Online Resource
    Cambridge University Press (CUP) ; 2008
    In:  Journal of Fluid Mechanics Vol. 601 ( 2008-04-25), p. 365-379
    In: Journal of Fluid Mechanics, Cambridge University Press (CUP), Vol. 601 ( 2008-04-25), p. 365-379
    Abstract: An incompressibility approximation is formulated for isentropic motions in a compressible stratified fluid by defining a pseudo-density ρ* and enforcing mass conservation with respect to ρ* instead of the true density. Using this approach, sound waves will be eliminated from the governing equations provided ρ* is an explicit function of the space and time coordinates and of entropy. By construction, isentropic pressure perturbations have no influence on the pseudo-density. A simple expression for ρ* is available for perfect gases that allows the approximate mass conservation relation to be combined with the unapproximated momentum and thermodynamic equations to yield a closed system with attractive energy conservation properties. The influence of pressure on the pseudo-density, along with the explicit ( x , t ) dependence of ρ* is determined entirely by the hydrostatically balanced reference state. Scale analysis shows that the pseudo-incompressible approximation is applicable to motions for which ${\cal M})$ 2 ≪ min(1, ${\cal R})$ 2 , where ${\cal M})$ is the Mach number and ${\cal R}$ the Rossby number. This assumption is easy to satisfy for small-scale atmospheric motions in which the Earth's rotation may be neglected and is also satisfied for quasi-geostrophic synoptic-scale motions, but not planetary-scale waves. This scaling assumption can, however, be relaxed to allow the accurate representation of planetary-scale motions if the pressure in the time-evolving reference state is computed with sufficient accuracy that the large-scale components of the pseudo-incompressible pressure represent small corrections to the total pressure, in which case the full solution to both the pseudo-incompressible and reference-state equations has the potential to accurately model all non-acoustic atmospheric motions.
    Type of Medium: Online Resource
    ISSN: 0022-1120 , 1469-7645
    Language: English
    Publisher: Cambridge University Press (CUP)
    Publication Date: 2008
    detail.hit.zdb_id: 1472346-3
    detail.hit.zdb_id: 218334-1
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  • 8
    Online Resource
    Online Resource
    Wiley ; 2019
    In:  Quarterly Journal of the Royal Meteorological Society Vol. 145, No. S1 ( 2019-09), p. 57-74
    In: Quarterly Journal of the Royal Meteorological Society, Wiley, Vol. 145, No. S1 ( 2019-09), p. 57-74
    Abstract: The sensitivity of ensemble simulations of deep convective events in the southeastern United States to initial‐condition (IC) errors is examined by imposing idealized moisture perturbations at small and large scales. Four severe weather events are considered, ranging from a springtime frontal system to convection driven almost exclusively by daytime heating. Events with strong synoptic‐scale forcing were insensitive to the scale of IC errors, but weakly forced events exhibited greater sensitivity to small‐scale than large‐scale IC errors. Additional ensemble simulations of idealized convective systems suggest that the greater sensitivity to small‐scale IC errors of the weakly forced cases arises from their higher sensitivity to the strength and location of the first convective elements. Ensemble spread and predictability are characterized by two measures: the ratio of the perturbation kinetic energy (KE) about the ensemble mean to the background KE and the neighborhood‐based fractions skill score (FSS) of hourly precipitation with respect to that in an unperturbed reference simulation. For simulations of both observed events and idealized convective systems, the FSS appears to be a more discriminating indicator of differences in predictability between different convective events.
    Type of Medium: Online Resource
    ISSN: 0035-9009 , 1477-870X
    URL: Issue
    RVK:
    RVK:
    Language: English
    Publisher: Wiley
    Publication Date: 2019
    detail.hit.zdb_id: 3142-2
    detail.hit.zdb_id: 2089168-4
    SSG: 14
    Location Call Number Limitation Availability
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  • 9
    Online Resource
    Online Resource
    Wiley ; 2021
    In:  Quarterly Journal of the Royal Meteorological Society Vol. 147, No. 738 ( 2021-07), p. 2691-2708
    In: Quarterly Journal of the Royal Meteorological Society, Wiley, Vol. 147, No. 738 ( 2021-07), p. 2691-2708
    Abstract: Linear theory has long been used to study mountain waves and has been successful in describing much of their behaviour. In the simplest theoretical context, that of two‐dimensional steady‐state flow with constant Brunt–Väisälä frequency ( N ) and horizontal wind speed ( U ), finite‐amplitude effects are relatively minor until wave breaking occurs. However, in more complex environmental profiles, significant finite‐amplitude effects occur below the wave‐breaking threshold. We constructed a linearized version of a fully nonlinear time‐dependent model, thereby facilitating direct comparisons between linear and finite‐amplitude solutions in cases with upstream profiles representative of typical real‐world events. Beginning with the simplest profile that includes a tropopause, namely an environment with constant upstream wind speed and two layers of constant static stability, we progressively investigate more complex profiles that include vertical wind shear typical of the midlatitude westerlies. Our results demonstrate that, even without wave breaking, finite‐amplitude effects can play an important role in modulating the mountain‐wave amplitude and gravity‐wave drag. The modulation is a function of the tropopause height and is most pronounced when the cross‐ridge flow increases strongly with height.
    Type of Medium: Online Resource
    ISSN: 0035-9009 , 1477-870X
    URL: Issue
    RVK:
    RVK:
    Language: English
    Publisher: Wiley
    Publication Date: 2021
    detail.hit.zdb_id: 3142-2
    detail.hit.zdb_id: 2089168-4
    SSG: 14
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  • 10
    Online Resource
    Online Resource
    American Meteorological Society ; 1983
    In:  Monthly Weather Review Vol. 111, No. 3 ( 1983-03), p. 430-444
    In: Monthly Weather Review, American Meteorological Society, Vol. 111, No. 3 ( 1983-03), p. 430-444
    Type of Medium: Online Resource
    ISSN: 0027-0644 , 1520-0493
    RVK:
    Language: English
    Publisher: American Meteorological Society
    Publication Date: 1983
    detail.hit.zdb_id: 2033056-X
    detail.hit.zdb_id: 202616-8
    SSG: 14
    Location Call Number Limitation Availability
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