Cyril Touzé

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Plates and shells



Non-linear dynamics of thin plates and shells with large-amplitude motions (geometrical non-linearity), is studied. The Von Karman stress-strain relationship is used, giving rise to the so-called analog dynamic of Von karman model for plates, and Donnell-Mushtari-Vlasov models for shells. A particular emphasis is put on the loss of stability of unimodal solutions. Internal resonance relationships are curcial in order to explain energy exchange and appearance of multimodal solutions.

Cicular plates

Due to the rotational symmetry, 1:1 resonances exist for every asymmetric mode. The coupling creating by this internal resonance has been studied theoretically and experimentally. Below is shown a frequency-reponse curve in the vicinity of the 1:1 resonance, showing the coupling between the two configurations.

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Shells

The case of a shallow psherical shell has been studied both theoretically and experimentally. The particular case of a 1:1:2 internal resonance has been investigated and experimentally demonstrated, see the frequency-reponse curves below.



The type of non-linearity (hardening or softening behaviour) has been studied thanks to the NNMs formalism. Lastly, reduced-order models has been built for different panels and doubly-curved shells, with refined stress-strain relationship obtained by including in-plane inertia. Finally the case of circular cylindrical shell has been used to compare NNM reduction method to the Proper Orthogonal Decomposition (POD).
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Geometric imperfections

Geometric imperfections for circular plates and thin shells, have been studied in the framework of the PhD thesis of Cédric Camier (defended on February 2, 2009). Below is shown an operating deflection shape experimentally measured on a shallow shell in the lab (left), for mode (0,2). It is compared to the prediction given by a perfect shell model, center. The geometric imperfections are in this case of the order of the thickness (1 mm), they have been measured and inserted into an imperfect shell model, predicting the mode shape shown right.

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Transition to chaos

The transition from periodic to chaotic vibrations is studied for thin circular plates with a free edge, in the framework of the models used to study the first transition, ie by using a modal procedure for discretizing the PDEs of motion. The ail is to reproduce numerically the transition scenario that is generically observed for thin shells, see the page on gongs and cymbals. A Gear's BDF procedure is used for integrating the resultants equations of motion in time, taht is needed to face the numerical stiffness of the problem. results are presented with Poincaré's stroboscopic cross-section. Below, the case of an imperfect plate showing a period-doubling before the onset of chaos.


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