Non-dimensional free surface elevation (with respect to the amplitude of oscillation A of the cylinder) as a function of non-dimensional time, computed at numerical gages located at x g = 2?/3 ( ) and 4?/3 ( ) from the cylinder, for two submergence depths z 0 of the cylinder : (a) -0.5 m ; (b) -0, p.37 ,
vertical (right) non-dimensional exciting forces as a function of kR, for incident waves of various steepnesses : H/? = 0, 05% ( ), 0.10% ( ), 0.20% ( ), 0.50% ( ), 1.00% ( ), p.69 ,
vertical (right) non-dimensional displacement of the center of mass as a function of kR, for incident waves of various steepnesses : H/? = 0 ( ), compared to Evans linear prediction ( ), 50% ( ), 1.00% ( ), 2.00% (, p.75 ,
La théorie linéaire d'Evans correspond à la courbe en trait plein, p.78 ,
On distingue au centre du cylindre le générateur et le système de guidage des fils électriques, et de chaque côté les deux ressorts latéraux surmontés des boîtiers contenant les accéléromètres, p.83 ,
le poids M g , les efforts de pression hydrodynamique F h , les efforts F r dans la direction radiale et la traînée visqueuse F v, p.84 ,
élévations de surface libre enregistrées par les trois sondes s 1 , s 2 , s 3 disposées dans le canal (voir Fig. 5.23 pour la position relative des sondes), composante radiale de l'accélération du cylindre enregistrées par chacun des deux accéléromètres, puissance éléctrique mesurée, p.89 ,
H r en vagues régulières et la hauteur significative H m 0 en vagues irrégulières en fonction de ?, pour f p = f r = f 0 = 1.65 Hz, d'après la théorie linéaire en profondeur finie, p.96 ,
65 Hz) pour H r = 1 cm et 4 valeurs de ?, tronqués sur l'intervalle [ f min f ma x ], p.96 ,
positions des deux cylindres et de la sonde s 1 . 16 cas sont considérés avec un écartement adimensionné d, p.101 ,
192 quadrilatères pour 194 noeuds En rouge : 2 noeuds à l'intersection de 3 arêtes qui perturbent la construction de l'élément glissant 4 × 4 noeuds (en noir), p.109 ,
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