Please use this identifier to cite or link to this item:
https://hdl.handle.net/10321/1225
DC Field | Value | Language |
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dc.contributor.author | McKenzie, J. F. | en_US |
dc.contributor.author | Webb, G. M. | en_US |
dc.date.accessioned | 2015-02-12T06:37:16Z | - |
dc.date.available | 2015-02-12T06:37:16Z | - |
dc.date.issued | 2014-11-24 | - |
dc.identifier.citation | McKenzie, 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.issn | 0309-1929 | - |
dc.identifier.issn | 1029-0419 | - |
dc.identifier.uri | http://hdl.handle.net/10321/1225 | - |
dc.description.abstract | Rossby 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.extent | 20 p | en_US |
dc.language.iso | en | en_US |
dc.publisher | Taylor and Francis | en_US |
dc.relation.ispartof | Geophysical and astrophysical fluid dynamics (Online) | en_US |
dc.subject | Rossby waves | en_US |
dc.subject | Azimuthal wind | en_US |
dc.subject | Fourier-Floquet | en_US |
dc.title | Rossby waves in an azimuthal wind | en_US |
dc.type | Article | en_US |
dc.publisher.uri | http://dx.doi.org/10.1080/03091929.2014.986473 | en_US |
dc.dut-rims.pubnum | DUT-004391 | en_US |
dc.identifier.doi | http://dx.doi.org/10.1080/03091929.2014.986473 | - |
item.fulltext | With Fulltext | - |
item.openairecristype | http://purl.org/coar/resource_type/c_18cf | - |
item.languageiso639-1 | en | - |
item.openairetype | Article | - |
item.grantfulltext | open | - |
item.cerifentitytype | Publications | - |
Appears in Collections: | Research Publications (Applied Sciences) |
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mckenzie_webb_2015_geo___astrophy_fluid_dynamics.pdf | 674.17 kB | Adobe PDF | View/Open |
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