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Propagation of a finite-amplitude potential vorticity front along the wall of a stratified fluid

Published online by Cambridge University Press:  10 October 2002

MELVIN E. STERN
Affiliation:
Department of Oceanography, Florida State University, Tallahassee, FL 32306, USAstern@ocean.fsu.edu
KARL R. HELFRICH
Affiliation:
Department of Physical Oceanography, Woods Hole Oceanographic Institution, Woods Hole, MA 02543, USAkhelfrich@whoi.edu

Abstract

A similarity solution to the long-wave shallow-water equations is obtained for a density current (reduced gravity = g′, Coriolis parameter = f) propagating alongshore (y = 0). The potential vorticity q = f/H1 is uniform in −∞ < x [les ] xnose(t), 0 < y [les ] L(x, t), and the nose of this advancing potential vorticity front displaces fluid of greater q = f/H0, which is located at L < y < ∞. If L0 = L(−∞, t), the nose point with L(xnose(t), t) = 0 moves with velocity Unose = √gH0 φ, where φ is a function of H1/H0, f2L20/gH0. The assumptions made in the similarity theory are verified by an initial value solution of the complete reduced-gravity shallow-water equations. The latter also reveal the new effect of a Kelvin shock wave colliding with a potential vorticity front, as is confirmed by a laboratory experiment. Also confirmed is the expansion wave structure of the intrusion, but the observed values of Unose are only in qualitative agreement; the difference is attributed to the presence of small-scale (non-hydrostatic) turbulence in the laboratory experiment but not in the numerical solutions.

Type
Research Article
Copyright
© 2002 Cambridge University Press

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