Efficient numerical simulation of time-harmonic wave equations - - PowerPoint PPT Presentation

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Efficient numerical simulation of time-harmonic wave equations - - PowerPoint PPT Presentation

Efficient numerical simulation of time-harmonic wave equations Prof. Tuomo Rossi M.Sc. Tuomas Airaksinen Dr. Dirk Pauly M.Sc. Anssi Pennanen Ph.Lic. Sami K ahk onen M.Sc. Jukka R abin a Ph.Lic. Sanna M onk ol a


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Efficient numerical simulation of time-harmonic wave equations

  • Prof. Tuomo Rossi
  • Dr. Dirk Pauly

Ph.Lic. Sami K¨ ahk¨

  • nen

Ph.Lic. Sanna M¨

  • nk¨

a M.Sc. Tuomas Airaksinen M.Sc. Anssi Pennanen M.Sc. Jukka R¨ abin¨ a Department of Mathematical Information Technology University of Jyv¨ askyl¨ a, Jyv¨ askyl¨ a, Finland

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Collaboration

The research group has active collaboration with, e.g.,

  • Dr. Erkki Heikkola

(Numerola Oy)

  • Dr. Jari Toivanen

(University of Stanford)

  • Prof. Roland Glowinski

(University of Houston)

  • Prof. Norbert Weck,
  • Prof. Karl Josef Witsch,
  • Prof. Axel Klawonn,
  • Dr. Oliver Rheinbach

(University of Duisburg-Essen)

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On-going research project with Department of Physics, University of Jyv¨ askyl¨ a: efficient simulation methods for modeling the fluid flow in porous materials.

  • K. Mattila, J. Hyv¨

aluoma, T. Rossi, M. Aspn¨ as, J. Westerholm, An efficient swap algorithm for the lattice Boltzmann method, Computer Physics Communications (2007).

  • K. Mattila, J. Hyv¨

aluoma, J. Timonen, T. Rossi, Comparison of implementations

  • f the lattice-Boltzmann method, Computers & Mathematics with Applications

(2008).

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Contents

Physical phenomena Mathematical model (partial differential equations) Discretization methods Efficient solvers Simulation results

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Applications on various fields of science and engineering

  • Fluid dynamics: computational acous-

tics, echo sounding,

  • Elastodynamics: deformation of elastic

structures, seismic waves,

  • Electromagnetics:

antenna applica- tions,

  • Medical and biological systems: mod-

eling the structure of human tissue (medical imaging), cochlea in the in- ner ear.

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Example of coupled time-harmonic wave equations: fluid-structure interaction

Structure domain Ωs

Γ Ωs Ωf

Fluid domain Ωf

−ω2ρsus − ∇ · σ(us) = gs in Ωs, −ω2 c2 p − ∇2p = gf in Ωf, ∂p ∂nf + ω2ρfus · ns = 0

  • n Γ,

σ(us)ns − pnf = 0

  • n Γ.
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Numerical simulation

  • Simulation tools are used to avoid dangerous, expensive and time-consuming ex-

periments.

  • Computer simulation is an efficient tool in testing and optimizing of model param-

eters.

  • The design process can be dramatically improved and the development cycle short-

ened with computer aided modeling.

  • Solving problems arising from real life applications demands a considerable amount
  • f time and memory

– need to use efficient methods, – utilization of modern parallel computing platforms (Playstation 3 CELL-processors, Nvidia CUDA graphics processors).

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Discretization methods

  • Traditionally: low-order Finite Element Method (FEM),

– Especially for heterogeneous materials, sufficient accuracy requires dense dis- cretization = ⇒ large-scale systems to be solved. – Solutions with high frequency suffer from numerical dispersion. – For time-harmonic wave equations it is challenging to construct efficient iterative solution techniques.

  • Novel approaches:

– element-based methods with higher-order polynomial basis, e.g., Spectral Element Method (SEM), – Discrete Exterior Calculus (DEC).

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Efficient solution techniques

  • Fictitious domain,

– The computational domain is embedded into a larger and simpler domain. – a tetrahedral finite element mesh, which is locally adapted to the bound- ary of the obstacle D [B¨

  • rgers -90].

– linear finite elements with mass lump- ing.

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Wave scattering by a submarine, 200 wavelenghts per diameter, 20 nodes per wavelenght.

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  • Domain decomposition,

– The computational domain is divided into subdomains. – Instead of solving the whole PDE-system, the problems in the subdomains are solved separately. – The sequence of the subproblems converge to the solution of the original prob- lem.

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  • Multigrid preconditioners

– Shifted-Laplacian operator (damped Helmholtz operator), BSL = −∇ ·

1 ρ(x)∇ − (β1 + β2i) k(x)2 ρ(x) , as a preconditioner. Vibrations in a crankshaft

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  • Exact controllability

– Searching for the periodic solution of the time-dependent wave equations. – Initial conditions e0 and e1 are the control variables, and we minimize

J(e0, e1,Y(e0, e1)) = 1 2

  • YN − e0

T K

  • YN − e0
  • + 1

2

∂YN

∂t − e1

T

M

∂YN

∂t − e1

  • .

– Y contains the nodal values and solves the system of wave equations in [0, T].

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Recent/selected journal publications

  • T. Airaksinen, E. Heikkola, A. Pennanen, J. Toivanen, An algebraic multigrid based shifted-Laplacian preconditioner for

the Helmholtz equation, Journal of Computational Physics (2007).

  • T. Airaksinen, E. Heikkola, J. Toivanen, Active noise control in a stochastic domain based on a finite element model,

Journal of Sound and Vibration (submitted).

  • T. Airaksinen, A. Pennanen, J. Toivanen, A damping preconditioner for time-harmonic wave equations in fluid and

elastic material, Journal of Computational Physics (2009).

  • T. Airaksinen, S. M¨
  • nk¨

a, Comparison between shifted-Laplacian preconditioning and controllability method for com- putational acoustics, Journal of Computational and Applied Mathematics (to appear).

  • R. Glowinski, T. Rossi, A mixed formulation and exact controllability approach for the computation of the periodic

solutions of the scalar wave equation. (I) Controllability problem formulation and related iterative solution’, C. R.

  • Math. Acad. Sci. Paris, (2006).
  • E. Heikkola, S. M¨
  • nk¨

a, A. Pennanen, T. Rossi, Controllability method for acoustic scattering with spectral elements, Journal of Computational and Applied Mathematics (2007).

  • E. Heikkola, S. M¨
  • nk¨

a, A. Pennanen, T. Rossi, Controllability method for the Helmholtz equation with higher order discretizations, Journal of Computational Physics (2007).

  • S. M¨
  • nk¨

a, Time-harmonic solution for acousto-elastic interaction with controllability and spectral elements, Journal

  • f Computational and Applied Mathematics, (to appear).
  • D. Pauly, Generalized Electro-Magneto Statics in Nonsmooth Exterior Domains, Analysis, (2007).
  • D. Pauly, Complete Low Frequency Asymptotics for Time-Harmonic Generalized Maxwell Equations in Nonsmooth

Exterior Domains, Asymptotic Analysis, (2008).