2010
DOI: 10.1007/978-3-642-12110-4_164
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Two-Layer Shallow Water Equations with Complete Coriolis Force and Topography

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Cited by 22 publications
(3 citation statements)
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“…We consider in this section the two-layer rotating shallow-water equations on the NT f -plane which were derived by Stewart & Dellar (2010). The flow is a barotropic Bickley jet (in the sense of absence of vertical shear) evolving in mid-latitudes in the northern hemisphere, such that the traditional Coriolis parameter is positive f > 0 and the NT Coriolis parameter is F = O( f ).…”
Section: Linear Stability Analysis In the Two-layer Modelmentioning
confidence: 99%
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“…We consider in this section the two-layer rotating shallow-water equations on the NT f -plane which were derived by Stewart & Dellar (2010). The flow is a barotropic Bickley jet (in the sense of absence of vertical shear) evolving in mid-latitudes in the northern hemisphere, such that the traditional Coriolis parameter is positive f > 0 and the NT Coriolis parameter is F = O( f ).…”
Section: Linear Stability Analysis In the Two-layer Modelmentioning
confidence: 99%
“…In particular, there are two materially conserved potential vorticities (Stewart & Dellar 2010): Inertial instability requires that the product of the (traditional) Coriolis parameter and the absolute vorticity be negative. As NT q i={1,2} differs by terms proportional to F from the traditional potential vorticities for which F = 0 in (2.8)-(2.9), the stability bounds may be altered.…”
Section: Equations Of Motion and Relevant Parametersmentioning
confidence: 99%
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