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Earthquake Engineering Research - HKU Libraries - The University ...

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482<br />

stiffness or coefficient of viscous damping, has recently drawn more attention [Kamopp, D., 1995, Dyke, S.<br />

J., Spencer, Jr., B. R, 1997, Yoshida. S. and Yoshida. K., 1997, Fujio. T. and Yoshida. K., 1999] than the<br />

active control methodology which needs much power. Semi-active control is characteristic of less power then<br />

active control and higher performance than passive control. Especially, variable dampers have already been<br />

put into practice in the field of automobile, and a skyhook damper is approximately realized by using variable<br />

damper. Since the suppression of actuator power is an important issue for active structural control, in this<br />

stud\, a new semi-active control method for vibration base isolation is presented by a sliding mode using the<br />

switching hyperplane designed by disturbance-accommodating bilinear control.<br />

One of the authors proposed an bilinear potimal control with feedforward link for a semi-active dynamic<br />

vibration absorber and then applied it to a base isolation problem [Fujio. T. and Yoshida. K., 1999]. This<br />

study presents a sliding mode controller using the switching hyperplane designed by disturbance-accommodating<br />

bilinear control. In order to investigate the performance and the effectiveness of the proposed method<br />

by numerical calculation and computer simulation, it is applied to a model of an actual structure with 10 degree-of-freedom.<br />

CONTROLLER DSEIGN<br />

Fundamental Model for Controller Design<br />

hi this study, a ten-storied structural model with semi-active base isolator subjected to seismic excitation is<br />

treated as a control object A variable damper is installed between the base and the first story of structure. As a<br />

result of the eigenvalueanalysis, first natural frequency of system is 0.25Hz and damping ratio is 2%, respectively.<br />

<strong>The</strong>n this control object is represented by the following bilinear equation.<br />

V" ;r Y" •' • A TC TC V • • • T I<br />

l A 0 A 10 "hj<br />

"S L A 10<br />

where .r is state variable vector and z is disturbance vector, u denotes the vector of the control input, that is, the<br />

damping coefficient of damper given by the semi-active control.<br />

Controller with Feedforwrad Link<br />

In this stud}, it is assumed that there is a disturbance with flat spectral density at the controlled frequency<br />

range in order to adapt to various earthquakes. Accordingly, by restricting the frequency range of disturbance,<br />

we assume that the characteristic of power sepectal density is the same as white noise within the restricted<br />

frequency range. <strong>The</strong>n, we assume that the disturbance is such a colored noise that has the transfer function of the<br />

characteristic of a low pass filter as shown in Fig. 1, whose transfer function is give by

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