Abstract
The common structure of a number of physical network systems is identified, based on the incidence structure of the graph, the weights associated to the edges, and the total stored energy. State variables may not only be associated to the vertices, but also to the edges of the graph; in clear contrast with multiagent systems. Structure-preserving model reduction concerns the problem of approximating a complex physical network system by a system of lesser complexity, but within the same class of physical network systems. Two approaches, respectively, based on clustering and on Kron reduction, are explored.
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Notes
- 1.
See for a further discussion [24].
- 2.
The setup can be easily extended (i.e., by using Kronecker products) to the situation that the scalar variable \(x_i\) is replaced by a vector in some higher dimensional physical space, e.g., \(\mathbb {R}^3\); see the remarks later on.
- 3.
Note that \(\mathscr {K}\), and therefore the Laplacian matrix \(\mathscr {L}= B \mathscr {K}B^T\), is dependent on the choice of the thermodynamic equilibrium \(x^*\). However, this dependence is minor: for a connected complex graph the matrix \(\mathscr {K}\) is, up to a positive multiplicative factor, independent of the choice of \(x^*\) [25].
- 4.
For an extension of these results to complex-balanced mass action kinetics reaction networks we refer to [15].
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van der Schaft, A. (2015). Physical Network Systems and Model Reduction. In: Belur, M., Camlibel, M., Rapisarda, P., Scherpen, J. (eds) Mathematical Control Theory II. Lecture Notes in Control and Information Sciences, vol 462. Springer, Cham. https://doi.org/10.1007/978-3-319-21003-2_11
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