Theoretical model for the onset condition of a steady hydraulic jump

A hydraulic jump constitutes a transition from supercritical to subcritical flow. At the jump a roller forms, the water level suddenly increases, the flow velocity reduces, and power is dissipated. The type of hydraulic jump varies with the upstream Froude number. Experimental observations showed that for Froude numbers below F1 = 4.5 the jump is unstable and oscillatory, and from this value onwards it becomes steady. In this article, a novel theoretical model of the hydraulic jump is described which allows the transition point to be determined theoretically. The simple model assumes the power dissipation to occur through a counteracting moment at the roller. With an extended momentum balance approach, where the moments instead of the forces acting on the control volume are considered, the limit point is determined at F1 = 4.4. This correlates well with the experimentally derived value given in the literature of F1 = 4.5.

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Publication Details

Journal
Journal of Hydraulic Research
Published
2025-03-04
DOI
https://doi.org/10.1080/00221686.2025.2468952
Citations
1
Primary Topic
Hydraulic flow and structures
Type
article
Field-Weighted Citation Impact
0.95

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article

Theoretical model for the onset condition of a steady hydraulic jump

Gerald Müller
1 citations
Journal of Hydraulic Research
Hydraulic flow and structures
0.95
article

Theoretical model for the onset condition of a steady hydraulic jump

Gerald Müller
article en
1 citations

Abstract

A hydraulic jump constitutes a transition from supercritical to subcritical flow. At the jump a roller forms, the water level suddenly increases, the flow velocity reduces, and power is dissipated. The type of hydraulic jump varies with the upstream Froude number. Experimental observations showed that for Froude numbers below F1 = 4.5 the jump is unstable and oscillatory, and from this value onwards it becomes steady. In this article, a novel theoretical model of the hydraulic jump is described which allows the transition point to be determined theoretically. The simple model assumes the power dissipation to occur through a counteracting moment at the roller. With an extended momentum balance approach, where the moments instead of the forces acting on the control volume are considered, the limit point is determined at F1 = 4.4. This correlates well with the experimentally derived value given in the literature of F1 = 4.5.

Journal of Hydraulic ResearchVol. 63(2)
University of Southampton (GB)
University of Architecture, Civil Engineering and Geodesy, University of Southampton
Openalex Percentile: Top 28%
Hydraulic flow and structures
0.95
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