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dc.contributor.authorFiedler, Franz
dc.contributor.authorPanofsky, Hans A.
dc.date.accessioned2017-06-09T14:39:03Z
dc.date.available2017-06-09T14:39:03Z
dc.date.copyright1970/12/01
dc.date.issued1970
dc.identifier.issn0003-0007
dc.identifier.otherams-23606.pdf
dc.identifier.urihttp://onlinelibrary.yabesh.ir/handle/yetl/4160186
dc.description.abstractThe kinetic energy of the atmosphere is not spread uniformly over all wavelengths but has certain preferred scales, with gaps in between. Typically atmospheric structures are either fully three dimensional with horizontal wavelengths of the order of 100 m to several kilometers, such as convection cells (including thunderstorms) and mechanically driven eddies; or they are quasi-two-dimensional with horizontal dimensions of order of thousands of km. The first group of systems derives its energy from Kelvin-Helmholtz and hydrostatic instability, which depends on vertical gradients of wind and temperature; the second group is associated with barotropic or baroclinic instability, which depends on horizontal gradients of temperature and wind. Aloft, the small-scale systems are relatively less frequent than near the ground; on the other hand, intermediate-scale systems seem to be more common.
dc.publisherAmerican Meteorological Society
dc.titleAtmospheric Scales and Spectral Gaps
dc.typeJournal Paper
dc.journal.volume51
dc.journal.issue12
dc.journal.titleBulletin of the American Meteorological Society
dc.identifier.doi10.1175/1520-0477(1970)051<1114:ASASG>2.0.CO;2
dc.journal.fristpage1114
dc.journal.lastpage1120
dc.treeBulletin of the American Meteorological Society:;1970:;volume( 051 ):;issue: 012
dc.contenttypeFulltext


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