Abstract
Non-linear vibrations of free-edge shallow spherical shells are investigated, in order to predict the trend of non-linearity (hardening/softening behaviour) for each mode of the shell, as a function of its geometry. The analog for thin shallow shells of von Kármán's theory for large deflection of plates is used. The main difficulty in predicting the trend of non-linearity relies in the truncation used for the analysis of the partial differential equations (PDEs) of motion. Here, non-linear normal modes through real normal form theory are used. This formalism allows deriving the analytical expression of the coefficient governing the trend of non-linearity. The variation of this coefficient with respect to the geometry of the shell (radius of curvature R, thickness h and outer diameter 2 a) is then numerically computed, for axisymmetric as well as asymmetric modes. Plates (obtained as R → ∞) are known to display a hardening behaviour, whereas shells generally behave in a softening way. The transition between these two types of non-linearity is clearly studied, and the specific role of 2:1 internal resonances in this process is clarified.
| Original language | English |
|---|---|
| Pages (from-to) | 678-692 |
| Number of pages | 15 |
| Journal | International Journal of Non-Linear Mechanics |
| Volume | 41 |
| Issue number | 5 |
| DOIs | |
| Publication status | Published - 1 Jun 2006 |
Keywords
- Hardening/softening behaviour
- Internal resonance
- Non-linear normal modes
- Shallow spherical shells
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