“…An n ‐DOF linear time‐invariant structural system is considered in terms of the mass, damping, and stiffness matrices M , C , and K , respectively. The general differential equations of motion can be expressed in the matrix form as where u ( t ), ( t ), and ( t ) are the vectors of time‐variant displacement, velocities, and accelerations, respectively; and f ( t ) is the time‐dependent vector of the external dynamic excitation forces; u 0 and denote the initial displacement and velocity conditions. …”