“…The dynamics of system n's links of variable length, shown in Fig. 5, are described by a system of nonlinear differential equations presented in vector-matrix form [71,72]: (4.11) Here κ = ϕ, ψ, l: ϕ = (ϕ 1 , …, ϕ n ) and ψ = (ψ 1 , …, ψ n ) are vectors of angular coordinates of lumped masses; l = (l 1 , …, l n ) is the vector of the lengths of the links; = diag( , …, ), = diag( , …, ) are diagonal matrices; M κ are generalized forces; A κ (ϕ, ψ, l), B κ (ϕ, ψ, l), D κ (ϕ, ψ, l), E κ (ϕ, ψ, l), and G κ (ϕ, ψ, l) are…”