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dc.contributor.authorAmbacher, Matthew R.
dc.contributor.authorWaite, Michael L
dc.date.accessioned2021-10-19 19:38:42 (GMT)
dc.date.available2021-10-19 19:38:42 (GMT)
dc.date.issued2020-02-01
dc.identifier.urihttps://doi.org/10.1175/JAS-D-19-0146.1
dc.identifier.urihttp://hdl.handle.net/10012/17654
dc.description© Copyright 2020 American Meteorological Society (AMS). For permission to reuse any portion of this work, please contact permissions@ametsoc.org. Any use of material in this work that is determined to be “fair use” under Section 107 of the U.S. Copyright Act (17 U.S. Code §?107) or that satisfies the conditions specified in Section 108 of the U.S. Copyright Act (17 USC § 108) does not require the AMS’s permission. Republication, systematic reproduction, posting in electronic form, such as on a website or in a searchable database, or other uses of this material, except as exempted by the above statement, requires written permission or a license from the AMS. All AMS journals and monograph publications are registered with the Copyright Clearance Center (https://www.copyright.com). Additional details are provided in the AMS Copyright Policy statement, available on the AMS website (https://www.ametsoc.org/PUBSCopyrightPolicy).en
dc.description.abstractNormal modes are used to investigate the contributions of geostrophic vortices and inertia–gravity waves to the energy spectrum of an idealized baroclinic wave simulation. The geostrophic and ageostrophic modal spectra (GE and AE, respectively) are compared to the rotational and divergent kinetic energy (RKE and DKE, respectively), which are often employed as proxies for vortex and wave energy. In our idealized f-plane framework, the horizontal modes are Fourier, and the vertical modes are found by solving an appropriate eigenvalue problem. For low vertical mode number n, both the GE and AE spectra are steep; however, for higher n, while both spectra are shallow, the AE is shallower than the GE and the spectra cross. The AE spectra are peaked at the Rossby deformation wavenumber kR n , which increases with n. Analysis of the horizontal mode equations suggests that, for large wavenumbers k kR n , the GE is approximated by the RKE, while the AE is approximated by the sum of the DKE and potential energy. These approximations are supported by the simulations. The vertically averaged RKE and DKE spectra are compared to the sum of the GE and AE spectra over all vertical modes; the spectral slopes of the GE and AE are close to those of the RKE and DKE, supporting the use of the Helmholtz decomposition to estimate vortices and waves in the midlatitudes. However, the AE is consistently larger than the DKE because of the contribution from the potential energy. Care must be taken when diagnosing the mesoscale transition from the intersection of the vortex and wave spectra; GE and AE will intersect at a different scale than RKE and DKE, despite their similar slopes.en
dc.description.sponsorshipFunding from the Natural Sciences and Engineering Research Council of Canada (Grant RGPIN-386456-2015)en
dc.language.isoenen
dc.publisherAMSen
dc.relation.ispartofseriesJournal of the Atmospheric Sciences;
dc.subjectBaroclinic flowsen
dc.subjectGravity wavesen
dc.subjectTurbulenceen
dc.subjectFourier analysisen
dc.subjectMesoscale modelsen
dc.subjectSpectral analysis/models/distributionen
dc.titleNormal Mode Spectra of Idealized Baroclinic Wavesen
dc.typeArticleen
dcterms.bibliographicCitationAmbacher, M. R., & Waite, M. L. (2020). Normal Mode Spectra of Idealized Baroclinic Waves. Journal of the Atmospheric Sciences, 77(3), 813–833. https://doi.org/10.1175/JAS-D-19-0146.1en
uws.contributor.affiliation1Faculty of Mathematicsen
uws.contributor.affiliation2Applied Mathematicsen
uws.typeOfResourceTexten
uws.peerReviewStatusRevieweden
uws.scholarLevelFacultyen


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