Summary
It is shown that the conservation equation of potential vorticity in the barotropic atmosphere\(\frac{d}{{dt}}\left( {\frac{{f + \zeta }}{{\Delta p}}} \right) = 0\) holds good, even in the baroclinic atmosphere, if it is permissible to introduce the isentropic and mass-conservation approximations.
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References
Charney J. G., 1948:On the Scale of Atmospheric Motions. Geof. Publ. 17, No. 2, 17 pp.
Charney, J. G., 1949:On a Physical Basis for Numerical Prediction of Large-Scale Motions in the Atmosphere. J. Meteor., 6, pp. 371–385
Haurwitz, B., 1941:Dynamic Meteorology. 1st. Ed., New York, Mc Graw-Hill Book Co, pp. 233–235.
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Arakawa, H. Rossby-Haurwitz's equation for the conservation of vertical vorticity component in the baroclinic atmosphere. Geofisica Pura e Applicata 18, 158–159 (1950). https://doi.org/10.1007/BF02000320
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DOI: https://doi.org/10.1007/BF02000320