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

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422<br />

(LQR/LQG), H M and the instantaneous optimal control strategies are frequently employed as active<br />

control and semi-active control strategies. However, the weighing matrices in the performance index<br />

are more difficult to choose. <strong>The</strong> stirrhess and mass matrices were ever proposed and widely used as<br />

the weighing matrix with the strain energy and kinetic energy of the controlled building being<br />

minimum in nature.<br />

However, damping matrix or stifihess matrix can be chosen as the linear quadratic objective weighing<br />

matrix for the instantaneous optimal control algorithm due to the special expression of the control<br />

force. <strong>The</strong> control force will provide a classical proportional damping to the controlled building when<br />

the mass multiplying by damping matrix (MC) is selected as the weighing of the instantaneous optimal<br />

control algorithm that results in a reasonable damping distribution for the controlled structures.<br />

Simulation results indicated that the control forces obtained from the instantaneous optimal control<br />

algorithm with the suggested weighing matrix can further reduce the drifts and absolute responses<br />

significantly than that obtained from the instantaneous optimal control algorithm with the conventional<br />

weighing matrix (MM) and LQR under the same control force. In addition, the control strategy is more<br />

suitable for semi-active variable damping control (such as variable damping damper and MR damper<br />

and ER damper) because it just acts like passive damper with adjustable parameters in nature. <strong>The</strong><br />

simulation results showed that the semi-active control based on the instantaneous optimal control<br />

algorithm with proposed weighing matrix is more trackable than that based conventional instantaneous<br />

optimal control and LQR strategies.<br />

2, INSTANTANEOUS OPTIMAL CONTROL WITH FULL STATE OBSERVER<br />

For a structure with n degrees of freedom (DOFs), the equation of motion is given by<br />

)= -MX S (f)+ DU(t) (2.1)<br />

whereMand Care the nxn mass and damping matrices, respectively, X(t),X(t),X(t) are the<br />

relative displacement, velocity and acceleration vectors, respectively, U(t) is the pxl active<br />

control force vector, D is the n x p distribution matrix that relates the effect of each control force<br />

with each DOF, X g (t) is the earthquake ground acceleration vector at each DOF, and F(x(t),X(t))<br />

is the restoring force of the structure and can be described by many hysteretic models, herein,<br />

Bouc-Wen model is employed to investigate the control strategy in this study as follows<br />

F(x(t\ X(t))= ofcc + (1 - a}kz (2.2)<br />

where k is the pre-yielding stiffiiess, a is the ratio of post-yielding stirrhess to pre-yielding<br />

stiffness, and (l-a)fc is the hysteretic part of the restoring force in which z is described by the<br />

following nonlinear differential equation<br />

~ (2.3)

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