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EULER Code for Helicopter Rotors EROS - European Rotorcraft Software Romuald Morvant March 2001
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PLAN 1- Presentation of the EROS project 2- The numerical SCHEMES 3- FUN & UNFACtored methods - RESULTS 4- CONCLUSIONS 5- FUTURE WORK
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OBJECTIVES Accurate prediction of the Aerodynamic Load distribution along the blades. 1- Reduce pilot control-loads 2- Increase speed 3- Identify and quantify the aerodynamic noise sources
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GEROS - GRID GENERATOR Adapted for Multi-blade calculations Various topologies in the framework of CHIMERA overlapping grids
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EROS - INVISCID EULER solver A- Cell-centred FINITE VOLUME method B- SPATIAL discretisation scheme C- DUAL-TIME implicit scheme D- TIME-STEPPING scheme
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Finite volume method 1- Closed surface 2- Rigid motion of the blade 3- Geometric Conservation Law
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Calculations of the surface fluxes
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IMPLICIT DUAL-TIME METHOD Redefinition of the Residual term Spatial discretisation Time discretisation
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Time-stepping SCHEME 1- Multi-stage Runge-Kutta scheme 2- Unfactored-factored method Use of acceleration techniques CFL number
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RESULTS from previous reports JAMESON - Runge-Kutta ROE - FUN method Preference for the ROE-FUN method: - BETTER respect of the physic (convection) - FASTER convergence
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FUN METHOD Factorisation in the spanwise direction 2 LINEAR SYSTEMS
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ANALYSES of the FUN method SMALL SIZE of the matrices LARGE NUMBER of pseudo-time steps to get a high convergence. Problems to damp out the small errors frequencies
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Objectif: SPEED the code UP 1- CODING 2- ALGORITHM UNFACtored method
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CODING UNROLLING of repetitive operations Transformation of the matrices (5x5) into a vector (25x1)
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ALGORITHM Implementation of the UNFACtored method Modification of the LHS block matrix size where the flow variables are stored Consideration of the 3 Dimensions
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REFERENCE TESTS - LANN WING : unsteady case (3D) - EC/ONERA 7A 4-bladed Model Rotor Model Rotor in transonic hover flight Single block grid
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UNSTEADY Case - LANN wing y/b=0.475 y/b=0.825 Sectional Force Coefficients Pitching moment coeff.
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UNSTEADY Case - LANN wing y/b=0.475 y/b=0.825 Mean Steady PressureFirst Harmonic Pressure
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Convergence behaviour STEADY run UNSTEADY run
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Periodic OH grid, 84 x 60 x 32 7A Model Rotor in hover flight
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Pressure Coefficient distribution, Normal force Coeff.
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CONVERGENCE Behaviour
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COMMENTARIES UNFACtored method Higher CFL number Faster convergence Higher average computing time / iterations
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FINAL RESULTS
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CONCLUSIONS GOOD agreement with the FUN method Calculations 5 times faster This method requires some other tests. It looks ATTRACTIVE for the unsteady cases
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FUTURE WORK Use of the UNFACtored method for the CHIMERA grid Implementation of the WENO method relevant to a future AEROACOUSTIC module: Blade Vortex Interaction (BVI) MPI implementation to enable the studies of large and important cases.
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