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EULER Code for Helicopter Rotors

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Aerodynamic Load distribution along the blades. 1- Reduce pilot control-loads. 2- Increase speed ... Adapted for Multi-blade calculations. Various topologies in ... – PowerPoint PPT presentation

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Title: EULER Code for Helicopter Rotors


1
EULER Code for Helicopter Rotors
EROS - European Rotorcraft Software
Romuald Morvant March 2001
2
PLAN
1- Presentation of the EROS project 2- The
numerical SCHEMES 3- FUN UNFACtored methods -
RESULTS 4- CONCLUSIONS 5- FUTURE WORK
3
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

4
GEROS - GRID GENERATOR
  • Adapted for Multi-blade calculations
  • Various topologies in the framework of
  • CHIMERA overlapping grids

5
EROS - INVISCID EULER solver
A- Cell-centred FINITE VOLUME
method B- SPATIAL discretisation scheme
C- DUAL-TIME implicit scheme D-
TIME-STEPPING scheme
6
Finite volume method
1- Closed surface 2- Rigid motion of the
blade 3- Geometric Conservation Law
7
Calculations of the surface fluxes
8
IMPLICIT DUAL-TIME METHOD
Time discretisation
Spatial discretisation
Redefinition of the Residual term
9
Time-stepping SCHEME
1- Multi-stage Runge-Kutta scheme
2- Unfactored-factored method
Use of acceleration techniques CFL number
10
RESULTS from previous reports
Ö JAMESON - Runge-Kutta Ö ROE - FUN
method Preference for the ROE-FUN method -
BETTER respect of the physic (convection) -
FASTER convergence
11
FUN METHOD
Factorisation in the spanwise direction
2 LINEAR SYSTEMS
12
ANALYSES of the FUN method
Ö SMALL SIZE of the matrices LARGE NUMBER
of pseudo-time steps to get a high
convergence. Problems to damp out the
small errors frequencies
13
Objectif SPEED the code UP
  • 1- CODING
  • 2- ALGORITHM
  • UNFACtored method

14
CODING
UNROLLING of repetitive operations Transformation
of the matrices (5x5) into a vector (25x1)
15
ALGORITHM
16
REFERENCE TESTS
  • - LANN WING unsteady case (3D)
  • - EC/ONERA 7A 4-bladed Model Rotor
  • Model Rotor in transonic hover flight
  • Single block grid

17
UNSTEADY Case - LANN wing
Pitching moment coeff.
Sectional Force Coefficients
y/b0.475
y/b0.825
18
UNSTEADY Case - LANN wing
Mean Steady Pressure
First Harmonic Pressure
y/b0.475
y/b0.825
19
Convergence behaviour
STEADY run
UNSTEADY run
20
7A Model Rotor in hover flight
Periodic OH grid, 84 x 60 x 32
21
7A Model Rotor in hover flight
Pressure Coefficient distribution, Normal force
Coeff.
22
CONVERGENCE Behaviour
23
COMMENTARIES
UNFACtored method Ö Higher CFL
number Ö Faster convergence Higher
average computing time / iterations
24
FINAL RESULTS
25
CONCLUSIONS
Ö GOOD agreement with the FUN method Ö
Calculations 5 times faster This method
requires some other tests. It looks
ATTRACTIVE for the unsteady cases
26
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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