IUTAM Symposium on Advances in Mathematical Modelling of Atmosphere and Ocean Dynamics pp 245-250 | Cite as
Physical Mechanisms of Nonlinear Equilibration of a Baroclinically Unstable Jet over Topographic Slope
Abstract
Spatio-temporal evolution of meanders on a baroclinically unstable jet over a topographic slope is investigated using pulse asymptotics and numerical simulations. An unperturbed jet is prescribed by a potential vorticity front in the upper layer overlaying intermediate layers with weak potential vorticity gradients and a quiescent bottom layer over a positive (same sense as isopycnal tilt) cross-stream topographic slope.
An initially localized meander evolves into a wave packet growing and propagating downstream. The pulse asymptotics oflinear waves allows to characterize the structure of amplifying baroclinic wave packets by spatio-ternporal modes which grow exponentially along some rays x/t=const but decay along other rays. In a fully nonlinear numerical solution the instability growth is compensated by the nonlinear terms and the central part of wave packet saturates. The upstream and downstream development ofthe disturbance near the leading and trailing edges ofthe wave packet obeys the linear wave theory.
For a weak bottom slope of0.002 the growth rate is only 10% less than that for a flat bottom. Nevertheless, meanders over a flat bottom are able to pinch offresembling warmand cold-core rings, while in the presence ofa weak bottom slope the maximum amplitudes of meanders and associated deep eddies saturate without eddy shedding.
-
It efficiently controls the nonlinear meander growth via constraining the development ofassociated deep eddies. The bottom slope modifies the evolution ofdeep eddies and causes their phase displacement in the direction ofthe upper layer troughs /crests, thus limiting growth ofthe meanders.
-
Behind the wave packet deep eddies form a nearly zonal circulation which stabilizes the jet. The main equilibration mechanism is homogenization ofthe lower layer potential vortic ity by deep eddies.
Keywords
Wave Packet Potential Vorticity Gulf Stream Flat Bottom Slope BottomPreview
Unable to display preview. Download preview PDF.
References
- Boss, E., and Thompson, L. (1999) Mean flow evolution of a barocl inically unstable potential vorticity front. J. Phys. Oceanogr., 29, 273–287.CrossRefGoogle Scholar
- Bush, A.E.G., McWilliams, J.C. and Peltier, W.R. (1995) The formation of oceanic eddies in symmetric and asymmetric jets. Part I: Early time evolution and bulk eddy transports. J. Phys. Oceanogr., 25, 1959–1979.CrossRefGoogle Scholar
- Farrell, B. F. (1982) Pulse asyrnptotics of the Charney baroclinic instability problem. J. Atmos. Sci, 39, 507–517.CrossRefGoogle Scholar
- Flierl, G. R. (1999) Thin jet and contour dynamics models of Gulf Stream meandering. Dyn. Atmos. Oceans, 29, 189–215.CrossRefGoogle Scholar
- Johns, W. E., Shay, T.J., Bane, J.M. and Watts, D.R. (1995 ) Gulf Stream structure, transport, and recirculation near 68° W. J. Geophys. Res, 100, 817–838.CrossRefGoogle Scholar
- Simmons, A.J., and Hoskins, B.J. (1978). The life cycles of of some nonlinear barocl inic waves. J. Atmos. Sci, 35, 414–423.CrossRefGoogle Scholar
- Lea, T., and Cornillon, P. (1996) Propagation of Gulf Sttream meanders between 75° and 45° W. J. Phys. Oceanogr., 26, 225–241.CrossRefGoogle Scholar
- Logoutov, O.G., Sutyrin, G.G., and Watts, D.R. (2000) Potential vort icity structure across the Gulf Stream: Observations and a PV-gradient model. J. Phys Oceanogr., 30.Google Scholar
- Mellor, G.L. (1998) Users guide for a three-dimensional, primitive equation, numerical ocean model. Atmos. and Oceanic Sciences Program, Princeton Univercity, 39 pp.Google Scholar
- Orlansky, L (1969) The influence of bottom topography on the stability of jets in a baroclinic fluid. J. Atmos. Sci, 26, 1216–1232.CrossRefGoogle Scholar
- Pierrehaumbert, R.T. and K. L. Swanson, K.L. (1995) Baroclinic Instability. Ann. Rev. Fluid Mech., 27, 419–467.CrossRefGoogle Scholar
- Sutyrin, G.G., Ginis, I. and Frolov, S.A. (2001) Equilibration of the Gulf Stream meanders and deep eddies over a sloping bottom. J. Phys. Oceanogr., 31.Google Scholar
- Swanson, K. and R. T. Pierrehumbert, R.T. (1994) Nonlinear wave packet evolution on a baroclinically unstable jet. J. Atmos. Sci, 51, 384–396.CrossRefGoogle Scholar
- Watts, D.R., Tracey, K.L, Bane, J.M. and Shay, T.J. (1995) Gulf Stream path and thermocline structure near 74° W and 68° W. J. Geophys. Res, 100, 18,291–18,312.CrossRefGoogle Scholar
- Wood, R. A. (1988) Unstable waves on oceanic fronts: Large amplitude behavior and mean flow generation. J. Phys. Oceanogr., 18, 75–787.CrossRefGoogle Scholar