The vertical structure of tidal currents and other oscillatory flows

160Citations
Citations of this article
76Readers
Mendeley users who have this article in their library.
Get full text

Abstract

Assuming a linearized equation of motion in the absence of stratification, the vertical structure of tidal currents is shown to be a function of two dimensionless parameters. The first of these, Y = (ω/E) 1 2D, is analogous to an Ekman height with ω the tidal frequency, D the depth, and E the (constant) vertical eddy viscosity. The second parameter, J = (ωE) 1 2/[(8/3π)k U ̄], introduces the effect of a quadratic bed stress through the bed-stress coefficient k and the depth-averaged velocity Ü. From these it is possible to illustrate the full range of possible vertical structure and to understand the basic scaling laws involved. By assuming E = a U ̄D good agreement between theory and observation was found. With this assumption vertical structure reduces to a function of just one parameter, namely kS, where S = U ̄2π/Dω is the Strouhal number. By resolving tidal current ellipses into clockwise and anticlockwise rotating components the original theory developed for recti-linear flow can be applied to fully three-dimensional flow. In this way, many of the observed characteristics of current structure in shallow seas may be explained. © 1982.

Cite

CITATION STYLE

APA

Prandle, D. (1982). The vertical structure of tidal currents and other oscillatory flows. Continental Shelf Research, 1(2), 191–207. https://doi.org/10.1016/0278-4343(82)90004-8

Register to see more suggestions

Mendeley helps you to discover research relevant for your work.

Already have an account?

Save time finding and organizing research with Mendeley

Sign up for free