The self-induced free-surface "swell flapping" caused by the interaction among a jet, a free surface and a structure

Citation
S. Someya et al., The self-induced free-surface "swell flapping" caused by the interaction among a jet, a free surface and a structure, J FLUID STR, 14(4), 2000, pp. 511-528
Citations number
5
Categorie Soggetti
Mechanical Engineering
Journal title
JOURNAL OF FLUIDS AND STRUCTURES
ISSN journal
08899746 → ACNP
Volume
14
Issue
4
Year of publication
2000
Pages
511 - 528
Database
ISI
SICI code
0889-9746(200005)14:4<511:TSF"FC>2.0.ZU;2-Y
Abstract
A new type of self-induced free-surface oscillation (swell flapping) was di scovered in a system with a jet, a free surface and a structure. An upward round jet was injected into a cylindrical tank from the bottom centre. The jet impinged on the bottom of an upper-inner-structure (UIS) in a LMFBR nuc lear reactor, which was set just beneath the free surface and above the jet inlet channel. The jet was separated at the edge of the UIS. In the cylind rical tank system, the effects of the geometric parameters on the occurrenc e and period of the swell flapping were investigated. The swell height duri ng the oscillation was thought to be important; therefore, the experiments were made with a rectangular tank system in order to measure the swell heig ht. Swell flapping was also observed in the rectangular tank. At a certain jet inlet velocity and UIS depth, the separated jet oscillated, forming a s well of the free surface around the UIS. The maximum swell height from the bottom edge of the UIS increases proportionately with the jet inlet velocit y, independently of the UIS depth. The period of oscillation increases with increasing swell height and velocity. The period of oscillation was divide d into a swell rising component and a swell breaking component. The time re quired for swell rising depended on the jet inlet velocity, while that requ ired for swell breaking corresponded to the wave propagation period. (C) 20 00 Academic Press.