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Clive Mingham, Ling Qian, Derek Causon and David Ingram

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Title: Clive Mingham, Ling Qian, Derek Causon and David Ingram


1
Clive Mingham, Ling Qian, Derek Causon and
David Ingram
Numerical Simulation of an OWSC Device Using a
Two-Fluid Free Surface Solver
Centre for Mathematical Modelling and Flow
Analysis, Manchester Metropolitan University, UK
2
Acknowledgements
  • EPSRC (UK) for funding the project
  • Joint project (wave tank model tests) with Prof.
    Trevor Whittaker and Dr. Matt Folley, Queens
    University of Belfast.

3
Talk Outline
  • Background
  • Numerics
  • Solver
  • Gridding
  • Results
  • Conclusions/future work

4
Background
  • Oscillating wave surge converter (OWSC) wave
    power device

5
Background
  • Accurate simulation of an OWSC can
  • provide
  • insight into the hydrodynamics
  • assessment of its performance
  • and needs to address
  • moving (water/air) free surfaces
  • complicated stationary and moving solid bodies

6
AMAZON-SC Numerical Features
  • Two fluid (water/air) free surface capturing
    solver based on the Cartesian cut cell mesh
  • Each fluid is identified by density
  • Solid stationary or moving bodies can be easily
    accommodated
  • MMU code written in-house.

7
Governing equations
  • 2D incompressible, Euler equations with variable
    density.

b is the coefficient of artificial compressibility
8
Discretisation
  • The equations are discretised using a finite
    volume formulation
  • Where Qi is the average value of Q in cell i
    (stored at the cell centre), Vi is the volume of
    the cell, Fij is the numerical flux across the
    interface between cells i and j and and Dlj is
    the length of side j.

9
Convective fluxes
  • The convective flux (Fij) is evaluated using
    Roes approximate Riemann solver.
  • To ensure second order accuracy, MUSCL
    reconstruction is used
  • where (x,y) is a point inside the cell ij, r is
    the coordinate vector of (x,y) relative to ij and
    DQij is the slope limited gradient.

10
Time discretisation
  • Euler implicit time discretisation is used
  • together with an artificial time variable t (to
    ensure a
  • divergence free velocity field) resulting in a
    linearised
  • RHS.

This system of linear equations is solved using
an approximate LU factorisation.
11
Boundary Conditions
  • Boundary conditions implemented include
  • Seaward boundary a solid moving paddle is used
    to generate waves (wave maker)
  • Atmospheric boundary a constant atmospheric
    pressure gradient is applied
  • Wall boundary for either vertical or horizontal
    walls at the domain boundary
  • Solid (moving) internal body modelled using
    Cartesian cut cell techniques

12
Cartesian Cut Cell Method
  • Automatic mesh generation
  • Boundary fitted
  • Extends to moving boundaries

13
Cartesian Cut Cells
  • Input vertices of solid boundary (and domain)

14
Cartesian Cut Cells
  • Input vertices of solid boundary (and domain)
  • Overlay background stationary Cartesian grid

15
Cartesian Cut Cells
  • Input vertices of solid boundary (and domain)
  • Overlay Cartesian grid
  • Identify Cut Cells and compute intersection
    points and other geometrical information.

16
The vane as a wave maker
Xa 170 mm, Ya 437 mm, Cl 20 mm, f 53
degrees water depth 200 mm, thickness of vane
25mm. wave probe positioned 500 mm to the left of
the vane
17
The vane as a wave maker
Rotation angle of the vane (from QUB test) as
input to the numerical simulation.
18
The vane as a wave maker
  • Water surface elevation at the probe position
    comparison with QUB tests

19
The vane as a wave maker
  • Animation showing velocity vectors and free
    surface position around the vane

20
OWSC Device Modelling
  • Flow conditions
  • Still water depth H 20 cm
  • Density of the vane m 1100 kg/m3
  • Wave period T 1.6 seconds
  • Velocity (horizontal) of wave maker
  • U -0.2 (1-e(-5t)) sin(2pt/T)
  • Angle of the backplane ? 45

21
OWSC Device Modelling
  • The motion of the vane is derived from the forces
    exerted on it by the surrounding water.

22
Conclusions
  • Initial results have been presented for
    simulation of the OWSC wave energy device using a
    surface capturing Cartesian cut cell method.
  • AMAZON-SC
  • Capable of modelling both water and air, as well
    as their interface
  • Can handle both static and moving boundaries
    easily.
  • The code shows promise for simulating a wide
    range of wave energy devices.

23
Future Work
  • Power takeoff simulation
  • 2D parametric study of the OWSC device
  • Extension to 3D with mesh adaptation
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