“…Accordingly, by substituting first ψ = g 1 and then ψ = g 2 in (21), together with the expression of V on,l and ω on,l given by (16) and (18), respectively, two independent equations in the unknowns δω n,l and ϕ n,l are obtained, whose solutions supply the two couples of frequency split and phase orientation (δω n,l , ϕ n,l ) relevant to the perturbed mode (n, l). Once the values of δω n,l and ϕ n,l have been computed, the corresponding modal shapes can be obtained by making use of the linear weak formulation (21).…”