Hostname: page-component-cd9895bd7-dk4vv Total loading time: 0 Render date: 2024-12-29T12:37:42.278Z Has data issue: false hasContentIssue false

The barotropic stability of the mean winds in the atmosphere

Published online by Cambridge University Press:  28 March 2006

Frank B. Lipps
Affiliation:
The Johns Hopkins University

Abstract

This paper considers the stability of a barotropic current on a beta earth. The motion is assumed to be horizontal, non-divergent and barotropic. The current is taken to be of the form U(y) = A sech2by+B. The perturbations are required to approach zero as y approaches ± ∞. We introduce the non-dimensional wave-number l and a parameter χ, which is a measure of the rotation effect. χ is inversely proportional to β.

There are only two kinds of perturbations: symmetric disturbances (those with maximum amplitude at y = 0) and antisymmetric disturbances (those with zero amplitude at y = 0). We find the neutral curve in the (χ, l2)-plane for both types of disturbances. The rates of amplification in the immediate vicinity of the neutral curves are also found. It is seen that the beta effect, which is due to the earth's rotation, tends to stabilize the current. For the symmetric disturbances we find a band of unstable wavelengths when χ > 1/2; and for large χ the estimated curve of the maximum value of the imaginary part of the phase velocity is asymptotic to the lower branch of the neutral curve. The antisymmetric disturbances are more stable than the symmetric disturbances.

Type
Research Article
Copyright
© 1962 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

Bateman Manuscript Project 1953 Higher Transcendental Functions, vol. I, chap. III. New York: McGraw-Hill.
Charney, J. G. 1947 The dynamics of long waves in a baroclinic westerly current. J. Met. 4, 13562.Google Scholar
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
Ince, E. L. 1944 Ordinary Differential Equations, chap. x. New York: Dover.
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
Lessen, M. & Fox, J. A. 1955 The stability of boundary layer type flow with infinite boundary conditions. 50 Jahre Grenzschichtforschung, pp. 1226. Braunschweig: Friedr. Vieweg und Sohn.
Lin, C. C. 1953 On the stability of the laminar mixing region between two parallel streams in a gas. NACA, Tech. Note 2887, pp. 2021.Google Scholar
Long, R. R. 1960 A laminar planetary jet. J. Fluid Mech. 7, 6328.Google Scholar
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.Google Scholar
Rossby, C. G. et al. 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
Schlichting, H. 1960 Boundary Layer Theory, pp. 1648. New York: McGraw-Hill.