Abstract

Abstract. In recent years coastal oceanographers have suggested using the "Strouhal" number or its inverse, the "Stokes" number, to describe the effect of bottom boundary layer turbulence on the vertical structure of both density and currents. These are defined as the ratios of the frictional depth (δ) to the water column depth (h) or vice versa. Although many researchers have mentioned that the effects of the earth's rotation should be important, they have tended to omit it. Rotation may have an important influence on tidal currents, as the frictional depth from a fully cyclonic to a fully anticyclonic tidal ellipse can vary by up to an order of magnitude at mid latitudes. The Stokes number might appear smaller for cyclonic current ellipses (larger for anticyclonic) than it is without rotation, resulting in frictional effects being underestimated (overestimated). Here, a way to calculate a Stokes number is proposed, in which the effect of the earth's rotation is taken into account. The standard Stokes and the rotational Stokes numbers are used as predictors for the position of the tidal mixing fronts in the Irish Sea. Results show that use of the rotational number improves the predictions of fronts in shallow cyclonic areas of the eastern Irish Sea. This suggests that the effect of rotation on the water column structure will be more important in shallow shelf seas and estuaries with strong rotational currents.

Highlights

  • Stokes (1851) studied the flow over an oscillating plate and defined the depth of frictional influence denoted by the parameter δ

  • Let us assume that we are in a shelf sea of about 30 m depth at latitude of 54◦ N, with a M2 tidal current that has a semi-major axis amplitude 1 ms−1 and an ellipticity that changes between −1 and 1

  • It is suggested that the Stokes number is the correct measure to be used concerning the ratio of the frictional depth to total depth as it is the ratio of the frictional to local accelerations

Read more

Summary

Introduction

Stokes (1851) studied the flow over an oscillating plate (analogous to oscillatory flow over the bottom) and defined the depth of frictional influence denoted by the parameter δ. The ratio of δ to the total water column depth (h) is known as the Stokes number: δ Stk = . The Stokes number can be expressed as follows: Stk = c1U∗ = δ . The Strouhal number was originally defined by Strouhal (1878) while experimenting with wires experiencing vortex shedding and singing in the wind. This number is used mainly to explain vortex shedding.

Objectives
Results
Conclusion
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.