manfred kaltenbacher in cooperation with a h ppe i sim
play

Manfred Kaltenbacher in cooperation with A. Hppe, I. Sim - PowerPoint PPT Presentation

Spectral finite elements for a mixed formulation in computational acoustics taking flow effects into account Manfred Kaltenbacher in cooperation with A. Hppe, I. Sim (University of Klagenfurt), G. Cohen and S. Imperial (INRIA, Paris) and B.


  1. Spectral finite elements for a mixed formulation in computational acoustics taking flow effects into account Manfred Kaltenbacher in cooperation with A. Hüppe, I. Sim (University of Klagenfurt), G. Cohen and S. Imperial (INRIA, Paris) and B. Wohlmuth (TU Munich) Alps-Adriatic University of Klagenfurt, Austria Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  2. Overview  Physical modeling  Pierce equation  Acoustic perturbation equation  FE formulation (no flow)  Acoustic conservation equations  Mixed formulation  Spectral elements  Comparison to wave equation with pFEM  FE formulation (with flow)  Acoustic perturbation equations  Occurring instabilities  Stabilization (flux term and dissipative term)  Application to aeroacoustics  Multi-Model approach Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  3. Acoustics in Flowing Media  Euler’s equations  Idea of decomposition Mean quantities Alternating quantities (disturbances) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  4. Acoustics in Flowing Media  Pierce equation (just for simple flows)  PML in time domain (Imbo Sim, Poster on Monday) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  5. Acoustics in Flowing Media  Acoustic perturbation equations 1  Subset of linearized Euler equations  Support just  acoustic modes  no entropy and vorticity modes  Fully considers  convection  refraction 1 R. Ewert and W. Schröder. Acoustic perturbation equations based on flow decomposition via source filtering. Journal of Computational Physics, 2003 Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  6. Acoustics (no flow)  Conservation equations  Linear acoustic wave equation Investigated Methods - h-FEM → mesh refinement - p-FEM & s- FEM → increase order of approximation Acoustic Conservation Equations Wave Equation Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  7. Acoustics (no flow)  Mixed formulation for conservation equations Lagrange polynomial space of order N  Discrete spaces 1 Mapping: Piola transform 1 G. Cohen & S. Fauqueux, Mixed Finite Elements with Mass-Lumping for the Transient Wave Equation Journal of Computational Acoustics, 2000 Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  8. Acoustics (no flow)  Properties of Piola transform  Preserves the normal component!  Term with gradient  Term with divergence Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  9. Acoustics (no flow)  Spectral finite elements Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  10. Acoustics (no flow)  Consequences of the Choice of Spaces  Elements  Semidiscrete Galerkin formulation Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  11. Acoustics (no flow)  Example  Excitation with a sine pulse of main wavelength λ  Reference solution obtained with h= λ/120 and Δt= 1/(f 200)  Computational mesh with mean element size of λ/5 and Δt<=λ /(2*c)  Time Stepping:  h-FEM & p-FEM: Implicit Newmark scheme  s-FEM: Explicit leapfrog time stepping Defomed mesh Setup Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  12. Acoustics (no flow)  Comparison Pressure Field Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  13. Acoustics (no flow)  Comparison for time domain computations Conservation equations Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  14. Acoustics Perturbation Equation  Formulation  Spaces Piola transform Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  15. Acoustics Perturbation Equation  Semidiscrete Galerkin formulation  Example  Initial condition  Flow Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  16. Acoustics in Flowing Media  Results (cartesian grid) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  17. Acoustics in Flowing Media  Results: Long time simulation (Cartesian grid) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  18. Acoustics Perturbation Equation  Formulation  Spaces Piola transform Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  19. Acoustics in Flowing Media  Stabilization  Central flux term  Reverse integration by parts on Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  20. Acoustics in Flowing Media  Stabilization  Averaging leads to  Add penalty (dissipative) term Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  21. Acoustics in Flowing Media  Results: Long time simulation (Cartesian grid, penalty term) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  22. Acoustics in Flowing Media  Results: Long time simulation (Cartesian grid, penalty + flux term) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  23. Acoustics in Flowing Media  Results: Long time simulation (deformed grid) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  24. Acoustics in Flowing Media  Results: Long time simulation (deformed grid, penalty term) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  25. Acoustics in Flowing Media  Results: Long time simulation (deformed grid, penalty + flux term) Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  26. Acoustics in Flowing Media  Results: Long time simulation (deformed grid) Spurious waves Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  27. Acoustics in Flowing Media  Shear flow Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  28. CAA (Computational Aeroacoustics)  Air foil  URANS CFD computations (Fluent, Michele Degenaro, AIT, Vienna)  Mach number about 0.3 Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  29. CAA (Computational Aeroacoustics)  Acoustic sources  Lighthill analogy Test function RHS of Lighthill’s equation Lamb vector  Acoustic Perturbation equation (APE) RHS of APE Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  30. CAA (Computational Aeroacoustics)  Arbitrary flow Without flow With flow Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  31. Multi-Model Approach  General idea PML layer Non-matching grid interface (Mortar framework) Acoustic perturbation equation Pierce equation Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  32. Multi-Model Approach  Interface conditions  Continuity of pressure  Continuity of normal component of particle velocity Lagrange multiplier Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  33. Multi-Model Approach  Formulation  Acoustic perturbation equation  Pierce equation  Continuity of pressure in a weak sense Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

  34. The End Thank you for your attention! Wave Propagation and Scattering, Inverse Problems and Applications in Energy and the Environment, RICAM, 2011

Recommend


More recommend