Hostname: page-component-cd9895bd7-fscjk Total loading time: 0 Render date: 2024-12-18T17:44:21.319Z Has data issue: false hasContentIssue false

The stability of an asymmetric zonal current in the atmosphere

Published online by Cambridge University Press:  28 March 2006

Frank B. Lipps
Affiliation:
Department of the Geophysical Sciences, The University of Chicago Present address: U.S. Weather Bureau, Washington, D.C.

Abstract

This paper considers the barotropic stability of an asymmetric zonal current on a rotating earth. The current is of hyperbolic tangent form in latitude. For this stability problem the neutral wave solutions are found and estimates of the growth rates for the unstable waves are obtained from the neutral solutions as in earlier investigations by the writer. It is again found that the beta effect which is due to the earth's curvature and rotation tends to stabilize the basic flow.

The stability of the basic flow is examined for a special case. For this case the current is centered at 35 degrees latitude, has a total shear of 30 m sec−1 and a half-width of 550 km. The most unstable waves are found to be wave-numbers 6 and 7 which amplify by a factor of e in 2·9 days. In addition, wave-numbers 5, 8 and 9 are also unstable. The stability of the symmetric jet is also examined for a comparable case. It is found that a wider band of wave-numbers is unstable. The most unstable wave is wave-number 8 which amplifies by a factor of e in 2·7 days.

In conclusion it is noted that these growth rates are slower than the amplification rates for the unstable waves associated with the baroclinic stability problem.

Type
Research Article
Copyright
© 1965 Cambridge University Press

Access options

Get access to the full version of this content by using one of the access options below. (Log in options will check for institutional or personal access. Content may require purchase if you do not have access.)

References

Charney, J. G. 1947 The dynamics of long waves in a baroclinic westerly current. J. Met. 4, 13562.Google Scholar
Drazin, P. G. 1958 The stability of a shear layer in an unbounded heteorogeneous inviscid fluid. J. Fluid Mech. 4, 21424.Google Scholar
Drazin, P. G. & Howard, L. N. 1962 J. Fluid Mech. 14, 25783.
Foote, J. R. & Lin, C. C. 1951 Some recent investigations in the theory of hydrodynamic stability. Quart. Appl. Math. 8, 26580.Google Scholar
Haurwitz, B. 1940 The motion of the atmospheric disturbances. J. Marine Res. 3, 3550.Google Scholar
Howard, L. N. 1963 Neutral curves and stability boundaries in stratified flow. J. Fluid Mech. 16, 33342.Google Scholar
Kuo, H. L. 1949 Dynamic instability of two-dimensional non-divergent flow in a barotropic atmosphere. J. Met. 6, 10522.Google Scholar
Kuo, H. L. 1951 Dynamic aspects of the general circulation and the stability of zonal flow. Tellus, 3, 26884.Google Scholar
Kuo, H. L. 1952 Three-dimensional disturbances in a baroclinic zonal current. J. Met., 9, 26078.Google Scholar
Lipps, F. 1962 The barotropic stability of the mean westerly winds in the atmosphere. J. Fluid Mech. 12, 397407.Google Scholar
Lipps, F. 1963 Stability of jets in a divergent barotropic fluid. J. Atm. Sci. 20, 12029.Google Scholar
Long, R. R. 1960 A laminar planetary jet. J. Fluid Mech. 7, 63238.Google Scholar
Michalke, A. 1964 J. Fluid Mech. 19, 54356.
Mintz, Y. 1955 Final computation of the mean geostrophic poleward flux of angular momentum and of sensible heat in the winter and summer of 1949. Article V, U.C.L.A. Final Report, March 1955, General Circulation Project, Contract AF 19(122)-48, Dept. Meteor.
Phillips, N. A. 1963 Geostrophic motion. Rev. Geophysics, 1, 12376.Google Scholar
Rossby, C.-G. and COLLABORATORS 1939 Relation between variations in the intensity of the zonal circulation of the atmosphere and the displacement of the semi-permanent centers of action. J. Marine Res. 2, 3855.Google Scholar
Wiin-Nielsen, A. 1961 On short and long term variations in quasi-barotropic flow. Mon. Wea. Rev. 89, 46176.Google Scholar