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Theoretical model for the onset condition of a steady hydraulic jump

Theoretical model for the onset condition of a steady hydraulic jump
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.
Education in hydraulic engineering, energy dissipation, hydraulic jump theory, hydraulic theory, open channel flow
0022-1686
278-282
Muller, Gerald
f1a988fc-3bde-429e-83e2-041e9792bfd9
Muller, Gerald
f1a988fc-3bde-429e-83e2-041e9792bfd9

Muller, Gerald (2025) Theoretical model for the onset condition of a steady hydraulic jump. Journal of Hydraulic Research, 63 (2), 278-282. (doi:10.1080/00221686.2025.2468952).

Record type: Article

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.

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Accepted/In Press date: 13 February 2025
e-pub ahead of print date: 28 March 2025
Published date: 2025
Keywords: Education in hydraulic engineering, energy dissipation, hydraulic jump theory, hydraulic theory, open channel flow

Identifiers

Local EPrints ID: 500531
URI: http://eprints.soton.ac.uk/id/eprint/500531
ISSN: 0022-1686
PURE UUID: 1fa9877e-7042-43ed-8b96-f36ab3f38a39
ORCID for Gerald Muller: ORCID iD orcid.org/0000-0003-1631-7777

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Date deposited: 02 May 2025 17:05
Last modified: 30 Aug 2025 01:41

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