Abstract

Abstract

Highlights

  • Hydraulic jumps are among the most iconic phenomena in fluid dynamics, found in a variety of situations ranging from thin films and kitchen sinks to large-scale open channels

  • Continuous hydraulic jumps in laminar channel flow the subcritical branch s−(h)

  • The hydraulic jumps in laminar or moderately turbulent open channel flow have been captured, complete with their mean-field shock structure, as stationary solutions of the generalized Saint-Venant equations

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Summary

Introduction

Hydraulic jumps are among the most iconic phenomena in fluid dynamics, found in a variety of situations ranging from thin films and kitchen sinks to large-scale open channels. The present paper deals with jumps on the intermediate scale where surface tension becomes insignificant, leaving gravitational and viscous effects as the two main factors Such jumps may be encountered in irrigation ditches or tilted channels on the laboratory scale under laminar or moderately turbulent flow conditions. This constitutes an extension of the classical first-order ‘backwater equation’ used to describe gradually varied flow (Rouse 1946).

The generalized Saint-Venant equations
Stationary wave solutions
Connection to the classical ‘backwater equation’
The dynamical system and its fixed point
Phase portraits of the hydraulic jumps
Overview of the four different jump types
Derivation of the jump length
Discussion of the expression for the jump length
Numerical experiment
Linear stability analysis: propagation and attenuation of small perturbations
Findings
Conclusion
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