Physical Mechanisms of Nonlinear Equilibration of a Baroclinically Unstable Jet over Topographic Slope

  • G. G. Sutyrin
  • I. Ginis
  • S. A. Frolov
Conference paper
Part of the Fluid Mechanics and Its Applications book series (FMIA, volume 61)

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.

Two physical mechanisms are important to understand the effects of topographic slope:
  • 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 Bottom 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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References

  1. 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
  2. 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
  3. Farrell, B. F. (1982) Pulse asyrnptotics of the Charney baroclinic instability problem. J. Atmos. Sci, 39, 507–517.CrossRefGoogle Scholar
  4. Flierl, G. R. (1999) Thin jet and contour dynamics models of Gulf Stream meandering. Dyn. Atmos. Oceans, 29, 189–215.CrossRefGoogle Scholar
  5. 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
  6. 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
  7. Lea, T., and Cornillon, P. (1996) Propagation of Gulf Sttream meanders between 75° and 45° W. J. Phys. Oceanogr., 26, 225–241.CrossRefGoogle Scholar
  8. 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
  9. 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
  10. 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
  11. Pierrehaumbert, R.T. and K. L. Swanson, K.L. (1995) Baroclinic Instability. Ann. Rev. Fluid Mech., 27, 419–467.CrossRefGoogle Scholar
  12. 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
  13. 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
  14. 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
  15. Wood, R. A. (1988) Unstable waves on oceanic fronts: Large amplitude behavior and mean flow generation. J. Phys. Oceanogr., 18, 75–787.CrossRefGoogle Scholar

Copyright information

© Springer Science+Business Media Dordrecht 2001

Authors and Affiliations

  • G. G. Sutyrin
    • 1
  • I. Ginis
    • 1
  • S. A. Frolov
    • 1
  1. 1.Graduate School of OceanographyUniversity of Rhode IslandNarragansettUSA

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