Identification of Continuous-Time Systems: Methodology and - download pdf or read online

By Ganti Prasada Rao, Naresh K. Sinha (auth.), N. K. Sinha, G. P. Rao (eds.)

ISBN-10: 9401055769

ISBN-13: 9789401055765

ISBN-10: 9401135584

ISBN-13: 9789401135580

In view of the significance of method identity, the overseas Federation of automated keep watch over (IFAC) and the foreign Federation of Operational learn Societies (IFORS) carry symposia in this subject each 3 years. curiosity in non-stop time techniques to procedure id has been growing to be lately. this can be obvious from the truth that the of invited classes on non-stop time structures has elevated from one within the eighth quantity Symposium that was once held in Beijing in 1988 to 3 within the ninth Symposium in Budapest in 1991. It was once through the eighth Symposium in August 1988 that the belief of bringing jointly vital effects relating to identity of continuing time platforms used to be conceived. a number of wonderful colleagues, who have been with us in Beijing at the moment, inspired us through promising immediate to give a contribution to a complete quantity of collective paintings. thus, we contacted colleagues around the globe, recognized for his or her paintings during this sector, with a proper request to give a contribution to the proposed quantity. The reaction was once recommended and overwhelmingly encouraging. We essentially thank all of the authors for his or her helpful contributions protecting a number of features of identity of continuing time systems.

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1983). A sum of harmonically related sinusoids (a multisine) is another possible excitation not requiring the explicit reconstruction of the time-derivatives. The transfer function of a TI linear system can be estimated using the method described in Pintelon and Schoukens (1990a), which is a maximum likelihood errors-in-variables method based on frequency-domain relations. Often it is not possible or too expensive to choose the excitation signal of the device under test (DDT) and the operating conditions impose an arbitrary excitation.

7) where the suffix "e" denotes exact system quantities. To assure that the spectral fitting error doesn't exceed a certain maximum, it is now a matter of upper bounding the magnitude of the relative errors on the right hand side of this expression. 1 The alias error. In order to simplify the exposition, the reasoning will be held for u(t) only. Identical considerations will be valid for yet). To control the spectral error due to alias, a first constraint on G(jro) and hence on AA(jro) emerges: G(jro) U(jro) must tend sufficiently fast to zero as I ro I increases beyond 1t, and this with respect to its behavior for I ro I < n.

Often it is not possible or too expensive to choose the excitation signal of the device under test (DDT) and the operating conditions impose an arbitrary excitation. Moreover, the observation of the excitation may be contaminated by noise of the same, if not a higher, level than the noise that corrupts the output. In that case, the above methods suffer from modeling errors or become unrealizable. To avoid the reconstruction of the time-derivatives, the differential equations are transformed into algebraiC equations via (multiple) integration with some weighting function.

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Identification of Continuous-Time Systems: Methodology and Computer Implementation by Ganti Prasada Rao, Naresh K. Sinha (auth.), N. K. Sinha, G. P. Rao (eds.)


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