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contributor authorWilloughby, H. E.
date accessioned2017-06-09T16:38:30Z
date available2017-06-09T16:38:30Z
date copyright2011/04/01
date issued2010
identifier issn0027-0644
identifier otherams-71432.pdf
identifier urihttp://onlinelibrary.yabesh.ir/handle/yetl/4213324
description abstractn gradient-balanced, cyclonic flow around low pressure systems, a golden radius exists where RG, the gradient-wind Rossby number, is ??1 = 0.618 034, the inverse golden ratio. There, the geostrophic, cyclostrophic, and inertia-circle approximations to the wind all produce equal magnitudes. The ratio of the gradient wind to any of these approximations is ??1. In anomalous (anticyclonic) flow around a low, the golden radius falls where RG = ?? = ?1.618 034, and the magnitude of the ratio of the anomalous wind to any of the two-term approximations is ?. In normal flow, the golden radius marks the transition between more-nearly cyclostrophic and more-nearly geostrophic regimes. In anomalous flow, it marks the transition between more-nearly cyclostrophic (anticyclonic) and inertia-circle regimes. Over a large neighborhood surrounding the golden radius, averages of the geostrophic and cyclostrophic winds weighted as ??2 and ??3 are good approximations to the gradient wind. In high pressure systems Rg, the geostrophic Rossby number, must be in the range 0 > Rg ≥ ?¼, and the pressure gradient cannot produce inward centripetal accelerations. An analogous radius where Rg = ???3 plays a role somewhat like that of the golden radius, but it is much less interesting.
publisherAmerican Meteorological Society
titleThe Golden Radius in Balanced Atmospheric Flows
typeJournal Paper
journal volume139
journal issue4
journal titleMonthly Weather Review
identifier doi10.1175/2010MWR3579.1
journal fristpage1164
journal lastpage1168
treeMonthly Weather Review:;2010:;volume( 139 ):;issue: 004
contenttypeFulltext


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