What is it about?

A simple diagnostic narrow channel shallow water model for the cross-channel distribution of the depth average velocity is developed. It is diagnostic, because the slope of the stream-wise free surface is specified and it models the cross-channel distribution of the depth average velocity without any knowledge of the velocity field. A non-dimensional parameter that encapsulates the channel dimensions and the relative importance of bottom friction to horizontal eddy viscosity is defined. Numerical solutions for the cross-channel distribution of the depth average velocity are obtained using values of this non-dimensional parameter for different cross-channel topographies. Numerical solutions for the depth average velocity are in turn used to find the cross-channel distribution for secondary flow and vertical velocity. Two-dimensional distributions of the vertical velocity in the n–z-plane show that changes in topography dominate the vertical velocity distribution. Three-dimensional tracers in a hypothetical open channel using scaling values from geophysical observations show that secondary circulation has a loose helical flow pattern of approximately one full rotation for every 360∘ of curvature. It is not unreasonable to suggest that this 1:1 relationship describes the looseness of secondary circulation in geophysical data.

Featured Image

Why is it important?

Helps build the body of knowledge of open channel flow.

Read the Original

This page is a summary of: A simple diagnostic model for the cross-channel distribution of the depth average velocity in curved open channels, Journal of the Royal Society of New Zealand, September 2020, Taylor & Francis,
DOI: 10.1080/03036758.2020.1803926.
You can read the full text:

Read

Contributors

The following have contributed to this page