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.
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CITATION STYLE
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
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