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FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle Development of an Integrated Computational Simulation Method for Fluid Driven Structure Movement and Acoustics I. Pantle Fachgebiet Strömungsmaschinen Karlsruher Institut für Technologie KIT

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  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Development of an Integrated Computational Simulation Method

    for Fluid Driven Structure Movementand Acoustics

    I. Pantle

    Fachgebiet StrömungsmaschinenKarlsruher Institut für Technologie

    KIT

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    FSI can be:Structural vibrations excite fluid waves/acoustical waves in fluidsFluid flow excites structural vibrations which in turn excite acoustical waves

    Fluid flow excites structural deformations which hold an equilibrium state

    Motivation

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    FSI

    Motivation/Context

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Hybrid IntegratedApproach

    Hybrid = 2 specialized codesfor CFD and CSD

    Integrated = 1 code for bothsimulation types

    Hybrid Approach

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Advantages/Disadvantages

    Border region must be treated with a specific approach to avoid singularities

    Grid movement on CFD side requires correction terms due to cell deformation

    1 grid possible, however, two sets of conservation equations valid for fluid and

    structure

    2 grids, one for CFD and CSD each, cell search and interpolation algorithm necessary

    For CFD typically Euler formulation: describes fluid state and its changes within control volumeFor CSD typically Lagrangian formulation: describes movement of control unit rather than its

    interior state

    One code for both fluid simulations and structural simulations

    Codes for CFD and CSD are highly adapted for specific problem

    Integrated ApproachHybrid Approach

    Hybrid Approach

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Characteristics of CFD and CSD Solver

    Covering plane stress, plate bending, axis symmetric and spatial structures

    Laminar, Reynolds-Averaged Navier-Stokes turbulence modeling, Large Eddy Simulation

    with various sub-grid scale models

    Fast Cholesky solver with Jennings storageContains driving interface for FSI:

    Sparse matrix iterative solver with Conjugate Gradient preconditioning (for very large

    structures)

    FSI-interfaces organizes cell-to-cell search algorithm on contact faces of fluid and

    structural mesh, manages interpolation of loads to the CSD side and of grid deformations

    back to the CFD side

    Direct sparse matrix with multi-cpu supportWith unsteady CFD simulations: FSI-interface manages temporal exchange

    3 types of solvers:Parallelized with MPICH

    Finite Element structural code (about 20 element types possible)

    Compressible Navier-Stokes, block-structured Finite Volume code

    CSD: Z88 (Univ. of Bayreuth)CFD: SPARC-FNX (KIT)

    Hybrid Approach

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Steady and UnsteadyApproach

    Steady Approach: for equilibriumdeformations (inner red part)

    Unsteady Approach: for vibrations(whole chart)

    Unsteadyness

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Contact Surfaces of Grids

    - 2 different cell distributions- interpolation of fluid loads to the solid structure (CFD to CSD)- interpolation of the structure deformations to the CFD grid (CSD to CFD) - unsteady case: interpolation of contact surface velocities

    Grid-to-grid Interpolation

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Curvature createserrors to some extent!

    Interpolation errorsGeometrical gaps

    Grid-to-grid Interpolation

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Steady flow through elastic pipeline

    Blue: CFD gridBrown: CSD grid

    Steady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Reduction of degrees of freedom: translational movement of pipeline not allowed

    Laminar flow, ideal gasType

    Young modulus: 1.1 MPaPoisson ration: 0.44

    No slip at wallsStatic pressure ps=104,755 PaMass flow rate: 0.13*104

    Data

    69,167 nodesNodes

    329.876 tetrahedons552,960 hexahedonsCells

    CSDCFD

    Steady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Steady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Developed fluid flow – before FSI is started: solid structure not deformed

    Some iterations after FSI is started: solid structure as well as flow profileis deformed

    Steady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Sequence until equlibrium stated betweenfluid loads and structural tension is reached

    Comparision of external structural diameter at equilibrium versus transmural pressure

    Steady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    2 types of interpolation: cell search algorithm starts from CFD side (upper) or from CSD side (lower) – cells on both sides of similar size

    Steady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    If CSD cell size much finer than CFD cell sizeAlternative interpolation (starting from CSD side) gives smoother fluid force distribution on the CSD contact face

    Conservative Interpolation

    Alternative Interpolation

    Steady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Elastic plate mounted behind square cylinder in crossflow: vortex street excites elastic plate’s vibrations

    Unsteady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    No reduction of degrees of freedom except for the mounting of the plate at the cylinder

    Laminar flow, ideal gasFlow Type

    Young modulus: 1.0 MPaPoisson ration: 0.35

    No slip at wallsFarfield: U=0.512 m/sStatic pressure ps=98,888.72 PaPeriodic boundaries

    Data

    3,964 nodesNodes

    14,908 tetrahedons425,984 hexahedonsCells

    CSDCFD

    Unsteady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    One period Tof vibration:

    ¼ T steps

    Unsteady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    Unsteady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    - Unsteadiness for implicit time dependant scheme implemented- Test cases and validation still in progress- Preliminary validation according to Wood, C., Gil, A. J., Hassan, O., Bonet, J., 2008, A Partitioned Coupling Approach for Dynamic Fluid-Structure Interaction with Applications to Biological Membranes, International Journal for Numerical Methods in Fluids, Vol. 57, Issue 5, pp. 555-581 - At present, Young modulus at 106 Pa for stabilization of the simulation, should be at 105 Pa - At present, amplitude of plate vibration at 1.2 cm, should be at 0.5 cm - At present, frequency of plate vibration at 3 Hz, should be at 1 Hz

    Unsteady Example

  • FSM – FSI – 21.05.2010 – Dr.-Ing. Iris Pantle

    FSI simulation tool created by attachingZ88 to SPARC

    Unsteady and steady simulations possible

    Still, algorithm verification and validation not yet terminated

    Validating measurements in progress; present validation data from other simulations

    Conclusions