Please use this identifier to cite or link to this item: https://hdl.handle.net/10321/1225
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dc.contributor.authorMcKenzie, J. F.en_US
dc.contributor.authorWebb, G. M.en_US
dc.date.accessioned2015-02-12T06:37:16Z-
dc.date.available2015-02-12T06:37:16Z-
dc.date.issued2014-11-24-
dc.identifier.citationMcKenzie, J.F. and Webb, G.M. 2014. Rossby waves in an azimuthal wind. Geophysical & Astrophysical Fluid Dynamics. 109(1) : 21-38.en_US
dc.identifier.issn0309-1929-
dc.identifier.issn1029-0419-
dc.identifier.urihttp://hdl.handle.net/10321/1225-
dc.description.abstractRossby waves in an azimuthal wind are analyzed using an eigen-function expansion. Solutions of the wave equation for the stream-function ψ for Rossby waves are obtained in which ψ depends on (r,φ,t) where r is the cylindrical radius, φ is the azimuthal angle measured in the β plane relative to the Easterly direction, (the β-plane is locally horizontal to the Earth’s surface in which the x-axis points East, and the y-axis points North). The radial eigenfunctions in the β-plane are Bessel functions of order n and argument kr,where k is a characteristic wave number and have the form anJn(kr) in which the an satisfy recurrence relations involving an+1, an,andan−1. The recurrence relations for the an have solutions in terms of Bessel functions of order n − ω/Ω where ω is the frequency of the wave and Ω is the angular velocity of the wind and argument a = β/(kΩ). By summing the Bessel function series, the complete solution for ψ reduces to a single Bessel function of the first kind of order ω/Ω. The argument of the Bessel function is a complicated expression depending on r, φ, a, and kr. These solutions of the Rossby wave equation can be interpreted as being due to wave-wave interactions in a locally rotating wind about the local vertical direction. The physical characteristics of the rotating wind Rossby waves are investigated in the long and short wavelength limits; in the limit as the azimuthal wind velocity Vw → 0; and in the zero frequency limit ω → 0 in which one obtains a stationary spatial pattern for the waves. The vorticity structure of the waves are investigated. Time dependent solutions with ω = 0 are also investigated.en_US
dc.format.extent20 pen_US
dc.language.isoenen_US
dc.publisherTaylor and Francisen_US
dc.relation.ispartofGeophysical and astrophysical fluid dynamics (Online)en_US
dc.subjectRossby wavesen_US
dc.subjectAzimuthal winden_US
dc.subjectFourier-Floqueten_US
dc.titleRossby waves in an azimuthal winden_US
dc.typeArticleen_US
dc.publisher.urihttp://dx.doi.org/10.1080/03091929.2014.986473en_US
dc.dut-rims.pubnumDUT-004391en_US
dc.identifier.doihttp://dx.doi.org/10.1080/03091929.2014.986473-
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item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.languageiso639-1en-
item.openairetypeArticle-
item.grantfulltextopen-
item.cerifentitytypePublications-
Appears in Collections:Research Publications (Applied Sciences)
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