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Uniform Asymptotics for the Linear Kelvin Wave in Spherical Geometry
Author(s) -
John P. Boyd,
Cheng Zhou
Publication year - 2008
Publication title -
journal of the atmospheric sciences
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.853
H-Index - 173
eISSN - 1520-0469
pISSN - 0022-4928
DOI - 10.1175/2007jas2356.1
Subject(s) - kelvin wave , wavenumber , physics , limit (mathematics) , equatorial waves , rossby wave , normal mode , plane (geometry) , classical mechanics , mathematical analysis , geometry , mathematics , meteorology , quantum mechanics , equator , atmospheric sciences , vibration , astronomy , latitude
The Kelvin wave is the gravest eigenmode of Laplace’s tidal equation. It is widely observed in both the ocean and the atmosphere. In the absence of mean currents, the Kelvin wave depends on two parameters: the zonal wavenumber s (always an integer) and Lamb’s parameter ε. An asymptotic approximation valid in the limit s2 + ε ≫ 1 is derived that generalizes the usual “equatorial wave” limit that ε → ∞ for fixed s. Just as shown for Rossby waves two decades ago, the width of the Kelvin wave is (ε + s2)−1/4 rather than ε−1/4 as in the classical equatorial beta-plane approximation.

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