Considers the axisymmetric balanced flow occurring in a thermally forced vortex in which the frictional inflow is confined to a thin boundary layer. Above the boundary layer the absolute angular momentum fR = rv + fr2 is conserved. R is the potential radius, ie the radius to which a particle must be moved (conserving absolute angular momentum) in order to change its tangential component v to zero. Using R as one of the dependent variables reviews the equations of the Eliassen balanced vortex model.-from Authors
CITATION STYLE
Schubert, W. H., & Hack, J. J. (1983). Transformed Eliassen balanced vortex model. Journal of the Atmospheric Sciences, 40(6), 1571–1583. https://doi.org/10.1175/1520-0469(1983)040<1571:TEBVM>2.0.CO;2
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