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Numerical Methods for Acoustic Problems with Complex Geometries Based on Cartesian Grids. D.N. Vedder 1103784. Overview. Computational AeroAcoustics Spatial discretization Time integration Cut-Cell method Results and proposals. CFD vs AeroAcoustics
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Numerical Methods for Acoustic Problems with Complex Geometries Based on Cartesian Grids D.N. Vedder 1103784
Overview • Computational AeroAcoustics • Spatial discretization • Time integration • Cut-Cell method • Results and proposals
CFD vs AeroAcoustics AeroAcoustics: Sound generation and propagation in association with fluid dynamics. Lighthill’s and Ffowcs Williams’ Acoustic Analogies Computational AeroAcoustics(AeroAcoustics)
Computational AeroAcoustics(Acoustics) • Sound modelled as an inviscid fluid phenomena Euler equations • Acoustic waves are small disturbances Linearized Euler equations:
Computational AeroAcoustics(Dispersion relation) • A relation between angular frequency and wavenumber. • Easily determined by Fourier transforms
Spatial discretization (DRP) • Dispersion-Relation-Preserving scheme • How to determine the coefficients?
Spatial discretization (DRP) • Fourier transform aj = -a-j
Spatial discretization (DRP) • Taylor series Matching coefficients up to order 2(N – 1)th Leaves one free parameter, say ak
Spatial discretization (DRP) 3. Optimizing
Spatial discretization (DRP) Dispersive properties:
Spatial discretization (OPC) • Optimized-Prefactored-Compact scheme • Compact scheme Fourier transforms and Taylor series
Spatial discretization (OPC) 2. Prefactored compact scheme Determined by
Spatial discretization (OPC) 3. Equivalent with compact scheme Advantages: 1. Tridiagonal system two bidiagonal systems (upper and lower triangular) 2. Stencil needs less points
Spatial discretization (OPC) • Dispersive properties:
Spatial discretization (Summary) • Two optimized schemes • Explicit DRP scheme • Implicit OPC scheme • (Dis)Advantages • OPC: higher accuracy and smaller stencil • OPC: easier boundary implementation • OPC: solving systems • Finite difference versus finite volume approach
Time Integration (LDDRK) • Low Dissipation and Dispersion Runge-Kutta scheme
Time Integration (LDDRK) • Taylor series • Fourier transforms • Optimization • Alternating schemes
Time Integration (LDDRK) Dissipative and dispersive properties:
Cut-Cell Method • Cartesian grid • Boundary implementation
Cut-Cell Method fn fe fw • fn and fw with boundary stencils • fint with boundary condition • fsw and fe with interpolation polynomials fint fsw
Test case Reflection on a solid wall • 6/4 OPC and 4-6-LDDRK • Outflow boundary conditions
Proposals • Resulting order of accuracy • Impact of cut-cell procedure on it • Richardson/least square extrapolation • Improvement of solution