PSI - Issue 62
E. Tomassini et al. / Procedia Structural Integrity 62 (2024) 903–910 Author name / Structural Integrity Procedia 00 (2019) 000–000
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2.1. Overview of the continuous SHM steps 2.1.1. Automated modal identification through the SSI-cov algorithm
The covariance-driven Stochastic Subspace Identification (SSI-cov) is a suitable choice for continuous SHM due to its easy automation, minimal parameter requirements, and capability to detect closely spaced frequency modes (Reynders, 2012). Let us consider a dynamic system represented by degrees freedom (DOFs) on which output signals are recorded at the sampling frequency � =1/Δ t , with Δt being the sampling time interval. The main steps of the modal identification through the SSI-cov algorithms are the following: Definition of the discrete time-state space model. The discrete time-state space model, representing the dynamic equilibrium of the system at discrete time instant k Δ t , with k being an integer, reads: ��� = � + � , � = � + � , (1) where ∈ ℝ ��×�� is the discrete state matrix, ∈ℝ �×�� is the output matrix, � , ��� ∈ ℝ �� are the state vectors at discrete time instant Δ and ( + 1)Δ , � ∈ ℝ � is the observation vector and � ∈ℝ �� and ∈ℝ � represent white noise processes accounting for the effect of unknown inputs modeled as stochastic processes, model inaccuracies and measuring noise. Computation of the Singular Value Decomposition (SVD) of the block Toeplitz correlation matrix. The block Toeplitz matrix is a square matrix containing the block output correlation matrices of the signals � ∈ ℝ �×� evaluated for positive time lags , = 1, … , (2 � −1) where � denotes the time-lag step. Therefore, the block-Toeplitz matrix reads: �|� � = ⎣ ⎢ ⎢ ⎡ R � � R � � �� R � � �� R � � … R � … R � ⋮ ⋮ R �� � �� R �� � �� …⋱ R ⋮ � � ⎦ ⎥ ⎥ ⎤ = � ∈ℝ � � �×� � � . (2) Given the factorization property of the correlation matrix, � = ��� = ��� E[ ��� �� ] , the following equations can be used to extract the observability and the controllability matrices : �|� � = , with = � ⋮ � � �� � = �/� , = [ � � �� … ] = �/� � . (3) Modal identification. Considering a system model order � (i.e. number of retained singular values in Eq. (3)), the matrices and in Eq. (1) can be extracted from the matrices and by mean of Eq. (3). Therefore, the modal matrix ∈ℝ �×� � and the eigenvalues matrix ∈ℝ �×� � of the structure for the discrete model can be evaluated from the eigenvalue decomposition of the matrix as: , = eig( ) where = [ � … � � ] , = � � ⋱ � � � (4) The eigenvalues � , natural frequencies � , damping ratios � , and modal matrix ∈ℝ �×� � of the continuos system can be evaluated as: � = ln � Δ , � = � 2 , ζ � = ( � || ) � || , = . (5) The process must iterate over various model orders ∈ [ , ] to assess the stability of the resulting modes, discriminating structural modes from spurious ones. After removing complex conjugate modes, the remaining ones are gathered in a stabilization diagram. Stable poles are identified by applying stability
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