“…The system identification problem investigated in this work can be defined as the determination of the corresponding system matrices A , B , C , D , Q ,and R (up to within a similarity transformation) using the input and output measurements available for N time steps, { u 1 , u 2 ,…, u N } and { y 1 , y 2 ,…, y N }. From the point of view of modal parameters, natural frequencies and modal damping ratios can be retrieved from the eigenvalues of A , the mode shapes can be evaluated using the eigenvectors of A and the output matrix C , and the modal masses can be computed using the eigenvectors of A and the input matrix B (see Cara for a general overview): - •The eigenvalues of A come in complex conjugate pairs, and each pair represents one physical vibration mode. Assuming proportional damping, the j th eigenvalue of A has the form where ω j are the natural frequencies, ζ j are damping ratios, and Δ t is the time step.
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