“…(16) can be written in a form with an autonomous periodic orbit by redefining the time variable according to (cf., 77 ) Here, θ is the phase of oscillation which gives a sense of the location along a stable periodic solution, ψ j is the j th isostable coordinate which gives a sense of the distance from the periodic orbit in a particular basis, ω = 2π/T is the natural frequency, κ j is the Floquet exponent associated with the j th isostable coordinate, Z(θ) and I(θ) are the phase and isostable response curves, respectively, which give the first order accurate dynamics, and B k (θ) and θ C ( ) , Δu(s) represents the deviation from the nominal input u(s). Information about the derivation of (22) and strategies for the numerical calculation of all necessary terms of the reduction can be found in both 24 and 25 . In the specific situation considered in this work, as a consequence of the periodic orbit in (22) being induced by the periodic forcing, phase and time are related according to θ(s) = ωs.…”