Toroidal vibrations of anisotropic spheres with spherical isotropy

This paper derives the exact frequency equation for the toroidal mode of vibrations for a spherically isotropic elastic sphere. The vibrations of spherically isotropic solids are solved by introducing two wave potentials (Phi and Psi) such that the general solutions for free vibrations can be classified into two independent modes of vibrations, namely the "toroidal" and "spheroidal" modes. Both of these vibration modes can be written in terms of spherical harmonics of degree n. The frequency equation for the toroidal modes is obtained analytically, and it depends on both n and beta [=(C-11 - C-12)/(2C(44))], where C-11, C-12, and C-44 have the usual meaning of moduli and are defined in Eqs. (2)-(3); and, as expected, Lamb's (1882) classical frequency equation is recovered as the isotropic limit. Numerical results show that the normalized frequency omega a/C-s increases with both n and beta, where omega is the circular frequency of vibration, a the radius of the sphere, and C-s is the shear wave speed on the spherical surfaces. The natural frequencies for spheres of transversely isotropic minerals and crystals, with beta ranging from 0.3719 to 1.8897, are also tabulated However; two coupled differential equations are obtained for the spheroidal modes, which remain to be solved.