1996
DOI: 10.1175/1520-0469(1996)053<0139:fratdo>2.0.co;2
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Flow Regimes and Transient Dynamics of Two-Dimensional Stratified Flow over an Isolated Mountain Ridge

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Cited by 56 publications
(53 citation statements)
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“…Pierrehumbert and Wyman, 1985), where N is the BruntÁVa¨isa¨la¨frequency, describing the buoyancy on a vertically displaced air parcel, h is the mountain height and U is the flow speed of the airmass impinging on the mountain (e.g. Peng et al, 1995;Tru¨b and Davies, 1995;Lin and Wang, 1996;Ó lafsson and Bougeault, 1996). High values of hˆfacilitate for blocked flow leading to more of the flow going around than over the mountain.…”
Section: Introductionsupporting
confidence: 69%
“…Pierrehumbert and Wyman, 1985), where N is the BruntÁVa¨isa¨la¨frequency, describing the buoyancy on a vertically displaced air parcel, h is the mountain height and U is the flow speed of the airmass impinging on the mountain (e.g. Peng et al, 1995;Tru¨b and Davies, 1995;Lin and Wang, 1996;Ó lafsson and Bougeault, 1996). High values of hˆfacilitate for blocked flow leading to more of the flow going around than over the mountain.…”
Section: Introductionsupporting
confidence: 69%
“…Some early theoretical studies (Long 1953;Miles and Huppert 1968) elucidated the nonlinear mechanisms for an early stage of the wave breaking processes. Understanding of these mechanisms has been significantly enriched through numerical experiments (Laprise and Peltier 1989;Lin and Wang 1996;Jiang et al 2004;McHugh and Sharman 2013). For a highly simplified case of uniform stratification and wind profile, a Mountain Froude number (cf.…”
Section: Accelerated Deposition Via Breaking Lee Wavesmentioning
confidence: 99%
“…Leewave breaking occurs when Fr is about equal to or smaller than unity (e.g. Lin and Wang 1996). The condition of Fr∼1 is not an unusual one; for example, if we take a climatological lapse rate of 0.006 K m −1 for the troposphere (NOAA 1976;Wallace and Hobbs 2006), which gives N≈0.0117 s −1 , a wind speed of U=12 m s −1 , and a mountain with h=1,000 m, the Mountain Froude number is Fr≈1.02.…”
Section: Accelerated Deposition Via Breaking Lee Wavesmentioning
confidence: 99%
“…In the literature, various flow regimes based on this parameter are described (e.g. Peng et al, 1995;Triib and Davies, 1995;Lin and Wang, 1996;Ó lafsson and Bougeault, 1996). Smith (1989) outlined three main flow regimes over simple 3-D mountains: Low values of Nh/U enable the flow to pass over the mountain without any stagnation, and typically gentle gravity waves are formed.…”
Section: Theorymentioning
confidence: 99%