TY - JOUR
T1 - Anelastic semigeostrophic flow over a mountain ridge
AU - Bannon, P. R.
AU - Pe-Cheng Chu, Chu
N1 - Copyright:
Copyright 2018 Elsevier B.V., All rights reserved.
PY - 1988
Y1 - 1988
N2 - Scale analysis indicates that five nondimensional parameters (R0 2, ε, μ, λ and kλ) characterize the disturbance generated by the steady flow of a uniform wind (U0, V0) incident on a mountain ridge of width a. Here μ = h0/HR is the ratio of the mountain height h0 to the deformation depth HR = fa/N where f is the Coriolis parameter and N is the static buoyancy frequency. The parameters λ = HR/H and kλ are the ratios of HR to the density scale height H and the potential temperature scale height H/k respectively. There are two Rossby numbers; ε = V0/fa, and R0 = U0/fa. If R0 2 ≤ 1, then the mountain-parallel flow is in approximate geostrophic balance and the flow is semigeostrophic. If the flow is anelastic (λ ≃ 1), no direct correspondence between the two approximations was found. However the anelastic effects are qualitatively similar for the two and lead to: i) an increase in the strength of the mountain anticyclone, ii) a reduction in the extent (and possible elimination) of the zone of blocked, cyclonic flow, iii) a permanent turning of the flow proportional to the mass of air displaced by the mountain, and iv) an increase in the ageostrophic cross-mountain flow. The last result implies an earlier breakdown of semigeostrophic theory for anelastic flow over topography. Apart from a strengthening of the cold potential temperature anomaly over the mountain, the presence of a finite potential temperature scale height (ie k nonzero) does not significantly alter the flow solution. -from Authors
AB - Scale analysis indicates that five nondimensional parameters (R0 2, ε, μ, λ and kλ) characterize the disturbance generated by the steady flow of a uniform wind (U0, V0) incident on a mountain ridge of width a. Here μ = h0/HR is the ratio of the mountain height h0 to the deformation depth HR = fa/N where f is the Coriolis parameter and N is the static buoyancy frequency. The parameters λ = HR/H and kλ are the ratios of HR to the density scale height H and the potential temperature scale height H/k respectively. There are two Rossby numbers; ε = V0/fa, and R0 = U0/fa. If R0 2 ≤ 1, then the mountain-parallel flow is in approximate geostrophic balance and the flow is semigeostrophic. If the flow is anelastic (λ ≃ 1), no direct correspondence between the two approximations was found. However the anelastic effects are qualitatively similar for the two and lead to: i) an increase in the strength of the mountain anticyclone, ii) a reduction in the extent (and possible elimination) of the zone of blocked, cyclonic flow, iii) a permanent turning of the flow proportional to the mass of air displaced by the mountain, and iv) an increase in the ageostrophic cross-mountain flow. The last result implies an earlier breakdown of semigeostrophic theory for anelastic flow over topography. Apart from a strengthening of the cold potential temperature anomaly over the mountain, the presence of a finite potential temperature scale height (ie k nonzero) does not significantly alter the flow solution. -from Authors
UR - http://www.scopus.com/inward/record.url?scp=0024190186&partnerID=8YFLogxK
UR - http://www.scopus.com/inward/citedby.url?scp=0024190186&partnerID=8YFLogxK
U2 - 10.1175/1520-0469(1988)045<1020:ASFOAM>2.0.CO;2
DO - 10.1175/1520-0469(1988)045<1020:ASFOAM>2.0.CO;2
M3 - Article
AN - SCOPUS:0024190186
SN - 0022-4928
VL - 45
SP - 1020
EP - 1029
JO - Journals of the Atmospheric Sciences
JF - Journals of the Atmospheric Sciences
IS - 6
ER -