1975
DOI: 10.1175/1520-0469(1975)032<0767:eobowp>2.0.co;2
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Effect of Baroclinicity on Wind Profiles and the Geostrophic Drag Law for the Convective Planetary Boundary Layer

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Cited by 117 publications
(99 citation statements)
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“…Specific humidity q and virtual potential temperature * are given by (Arya (1975), Zilitinkevich and Deardorff (1974), etc.) can be expressed by (3) (4) (5) where zi is the height of PBL to be described later, zo roughness height, and K Karman constant.…”
Section: Datamentioning
confidence: 87%
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“…Specific humidity q and virtual potential temperature * are given by (Arya (1975), Zilitinkevich and Deardorff (1974), etc.) can be expressed by (3) (4) (5) where zi is the height of PBL to be described later, zo roughness height, and K Karman constant.…”
Section: Datamentioning
confidence: 87%
“…It has been, however, suggested that u*/ f is not a relevant height scale for unstable condition, and the direct use of the actual height of PBL has been recommended and introduced in the recent works. Arya (1975) dealt with the unstable condition separating the convective cases for which the lowest inversion base was adopted as the PBL height from those cases having no remarkable inversion for which the level of *-minimum is used as the PBL height. Melgarejo and Deardorff (1974) examined the similarity functions based on the PBL height taken as the level of the discontinuity in constancy of vertical profiles of temperature and humidity which appears nearly around the base of inversion layer.…”
Section: Introductionmentioning
confidence: 91%
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“…insignificant horizontal gradients of surface temperature) then the conventional relation tan ϕG = −B0/[ln(u * /f z0)−A0] applies [27,28]. The lack of ϕG dependence can be interpreted as a sensible choice in the EWA model, given that the tan(ϕG) dependence is not proper for latitudes approaching the equator [29], and from the EWA's implicit assumption that (in the stability treatment) variations in dH would dominate those do to geostrophic turning. We also remind that near the equator the geostrophic wind becomes ill-defined (the boundary-layer depth implied by ln(u * /f /z0) becomes unphysically large), due to the dominant ABL balance arising not from the Coriolis force but from other mechanisms.…”
Section: A Appendix: Stability Perturbation Of Geostrophic Drag Law mentioning
confidence: 99%
“…Above the constant stress layers both the inflow and outflow cases reveal highly sheared environments. Under the well-mixed convective regime, * 32 wind shear is small, which agrees with the results of Arya and Wyngaard (1975) .…”
Section: So 31mentioning
confidence: 99%