Abstract

AbstractA numerical method is presented to accurately simulate paddle-generated impulse waves. An order-one implicit splitting scheme allows advection and diffusion phenomena to be decoupled. Advec...

Highlights

  • Impulse waves in natural lakes or reservoirs are generated by landslides or avalanches and may lead to great damage in Alpine valleys (Miller 1960; Schnitter and Weber 1964; Fuchs and Boes 2010; Brideau et al 2012; Carey et al 2012)

  • Plane impulse waves have been investigated at the Laboratory of Hydraulics, Hydrology and Glaciology (VAW), ETH Zurich, leading to a general description of the wave generation and propagation processes used to predict the main wave features as a function of the governing slide impact parameters

  • A paddle-generated wave in a tilted 3D cavity was used as a benchmark to determine the accuracy of the numerical scheme for solving free surface flows governed by the Navier–Stokes equations (NSEs)

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Summary

Introduction

Impulse waves in natural lakes or reservoirs are generated by landslides or avalanches and may lead to great damage in Alpine valleys (Miller 1960; Schnitter and Weber 1964; Fuchs and Boes 2010; Brideau et al 2012; Carey et al 2012). Transport of the volume fraction of liquid φ and of the velocity v is performed on an adaptive octree grid using a semi-Lagrangian scheme, enabling CFL numbers larger than 1. Interpolation from tetrahedral mesh to octree; the neighboring tetrahedra (shown here as triangles) of cell C, shown in dashed lines, are involved in the interpolation known at time step tn, which defines Ωn 1⁄4 fx ∈ Λ; φnðxÞ 1⁄4 1g, the approximation of ΩðtnÞ, the liquid domain at time tn.

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