“…In particular, for an ideal non-viscous acoustic fluid, the fluid-loaded structural modes are known to expediently decouple into two independent classes of vibrations, namely, the first-class (torsional or toroidal) modes that are associated to equi-volumetric motion, and the second-class (spheroidal) modes that are directly impelled by the fluid loading. This way, as it has also been demonstrated in Refs., 74,75 only the second class modes of structural vibrations associated with ( V 2,n , v 2,n ; n = 0,1, 2,3, . .…”