By Pieter Eykhoff

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N+1 n n+2 Ί 2η C M. ,Α η ' Ί Β], CA N,, n CA n-1 fact 1. , c m it follows that [ c p C , , , . . >cm>2îa^c^J - Lcx>c2» · · · »cmJ 't+2 y A t+3 of the Gedanken-Experiment with the state model H =C V H n+1 n 3. MINIMAL SINGLE-INPUT, SINGLEOUTPUT MODELS Firstly, to pass from the Gedanken-Experi­ ment to some minimal single-input, singleoutput (SISO) models, we start with some restrictions of the basic arrays. Secondly, in anticipation of the minimal SISO models and some transforms between them we present some facts.

Cxx t+l " " A t+1' = Ax,. + Bu,. "t+1 " ""t ' ""t and the Gedanken-Experiment on this model. Its carrier in the former sense was as follows: past y = A Bw where w is white zero-mean signal with intensity Q. We have to construct the filtered output y = Α-^Βηι(χ+ν) derived from y contaminated by white zeromean observation noise v which has intensity R. ). observed at times t+l+j The i-th column of the reachability matrix and the j-th row of the observability matrix were computed from the (i-l)th column and (j-1) row, respectively.

The ability to separate different objects is poor, thus the modeling brings no information. On the other end, with poor testing and an over-simplified characterization, the predic­ tability of the outputs, for any inputs, is not sufficient. Between these two extremes, there must be some "optimal1' model, capable of extracting from the measurements, all ^potential struc­ tural knowledge with the most discriminative structure. The more data we get, the more sophisticated the model we can afford. This entropy-like nature of the optimal model, makes modeling an endless problem.

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