4.7 Article

Experimental and numerical determination of the optimum configuration of a parabolic wave extinction system for flumes

Journal

OCEAN ENGINEERING
Volume 238, Issue -, Pages -

Publisher

PERGAMON-ELSEVIER SCIENCE LTD
DOI: 10.1016/j.oceaneng.2021.109748

Keywords

Reflection coefficient; Iribarren number; Extinction system; Reflection methods; Numerical model validation

Funding

  1. Research Groups of the UPV/EHU [GIU19/029]
  2. Basque Government [IT1314-19]
  3. Joint Research Laboratory on Offshore Renewable Energy (JRL-ORE)
  4. University of Basque Country

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In this study, the phenomenon of wave reflection was studied using a self-developed passive extinction system. Different types of waves were generated in the laboratory and the variation of the reflection coefficient was studied under various conditions. A numerical model based on Eulerian multiphase VOF was designed and validated to determine the minimum reflection coefficient values for each set of experiments.
In this work the phenomenon of the wave reflection has been studied using a self-developed passive extinction system. Twenty one type of waves were generated in the laboratory using a piston-type wave maker. The variation of the reflection coefficient, Kr, was studied at several depths (h [m] of 0.3, 0.4, and 0.5), periods (0.636 < T [s] < 1.526), wave heights (0.010 < H [m] < 0.064), slopes (3 < alpha [degrees] < 17) and vertical end positions of the extinction system (y(1) [m] and y(2) [m] defined by y(1) [m] and alpha [degrees]), covering the linear and non-linear regions of the Le Mehaute chart. In parallel, an unsteady numerical model based on the Eulerian multiphase VOF was designed and validated according to the free surface displacement, n(j), and the calculation of the Kr values. Both type of validations were successful so this model was used in order to determine Kr values at slopes [degrees] that could not be physically reached by the extinction system. The obtained results allowed to determine the minimum Kr values for each set of experiments and finding a useful non-dimensional relationship of Kr,(h-y(1))/lambda and Ir as a function of the dispersion parameter, kh.

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