The numerical eigensolver works with the steady-flow solution to determine the eigenvalues and eigenmodes corresponding to the fluid-structure interaction system directly. It does not require a time history of forces on blades and subsequent Fourier transformation to determine stability. Also, it avoids computationally expensive time-domain simulations of small perturbation responses, where several cycles of oscillation are required to determine the growth or decay of perturbations. With this new method, the computational savings over the existing frequency and time-domain nonlinear methods are of the order of 100 to 10,000. However, note that fundamentally this is a small perturbation (linear) aeroelastic analysis, although steady-flow nonlinearities are taken into account (e.g., blade thickness, blade camber, and shock waves).
In the present work, a numerical eigensystem solver, based on a Lanczos procedure, is applied to a two-dimensional, full-potential, cascade aeroelastic solver. Calculations are performed for a cascade geometry used in previous research. Frequency- and time-domain flutter calculations were previously performed for this configuration. The steady solution is first obtained, as required in all such calculations. Then, the numerical eigensystem solver is used to calculate eigenvalues.
The eigenvalues obtained from this new approach indicate whether the aeroelastic system is stable or unstable. A comparison of the results from this approach with those from existing flutter determination methods shows that the new approach predicts the correct flutter condition. It shows good agreement in flutter speed and flutter mode.
The numerical eigensystem analysis results in substantial computer time savings in comparison to the frequency- and time-domain solutions. It will allow the use of nonlinear, time-marching solvers in routine aeroelastic design analysis. Because of the modular nature of the numerical eigensystem solver, it can be readily adapted to other time-marching aeroelastic solvers with minimal additional effort required on the researchers' part.
| Flutter parameter | Frequency domain | Time domain | New method |
|---|---|---|---|
| Frequency | 0.265 | 0.262 | 0.239 |
| Velocity | 13.35 | 13.45 | 13.65 |
Last updated April 16, 1996
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