Active Control of Structures by Andre Preumont, Kazuto Seto

By Andre Preumont, Kazuto Seto

With energetic regulate of constructions , international pioneers current the state of the art within the concept, layout and alertness of lively vibration regulate. because the call for for prime functionality structural structures raises, so will the call for for info and innovation in structural vibration keep watch over; this ebook presents a good treatise of the topic that may meet this requirement. The authors introduce lively vibration regulate by using shrewdpermanent fabrics and constructions, semi-active regulate units and various suggestions thoughts; they then talk about issues together with tools and units in civil constructions, modal research, lively regulate of high-rise constructions and bridge towers, energetic tendon regulate of cable buildings, and energetic and semi-active isolation in mechanical buildings.

energetic regulate of constructions:

  • Discusses new kinds of vibration keep watch over equipment and units, together with the newly built reduced-order actual modelling technique for structural keep an eye on;
  • Introduces triple high-rise structures hooked up through lively keep watch over bridges as devised through Professor Seto;
  • Offers a layout procedure from modelling to controller layout for versatile buildings;
  • Makes prolific use of functional examples and figures to explain the themes and expertise in an intelligible demeanour.

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The stability condition is therefore gG(0)H(0) = g ω2f n i=1 bT φi φiT b μi ωi 2 < 1. 95) Note that it is independent of the structural damping in the system. Since the instability occurs for large gains which are not used in practice, the PPF can be regarded as unconditionally stable. Unlike the lead controller of the previous section which controls all the modes which belong to z < ωi < p and even beyond, the PPF filter must be tuned on the targeted mode (it is therefore essential to know the natural frequency accurately), and the OTE/SPH OTE/SPH JWBK269-01 September 26, 2008 13:57 Printer Name: Yet to Come 34 Active Damping authority on the modes with very different frequencies is substantially reduced.

At ω = ωi + δω, G(ω) is dominated by the contribution of mode i and its sign is sign φi (a )φi (s) = −sign[φi (a )φi (s)]. 71) At ω = ωi+1 − δω, G(ω) is dominated by the contribution of mode i + 1 and its sign is sign φi+1 (a )φi+1 (s) 2 ωi+1 − ω2 = sign[φi+1 (a )φi+1 (s)]. 72) − is Thus, if the two residues have the same sign, the sign of G(ω) near ωi+1 + opposite to that near ωi . By continuity, G(ω) must vanish somewhere − . 70) are not all positive, there is no guarantee that G(ω) is an increasing function of ω, and one can find situations where there is more than one zero between two neighboring poles.

Along the actuator blocked ( = 0). Note that these are larger than the open-loop poles in the IFF case, because the stiffness is infinite in this case. 26(c) is fixed, and with it the maximum damping. 27. 27. 26 Duality between the IFF and the lead (DVF) control configurations. (a) IFF architecture with displacement actuator, force sensor and positive integral force feedback. (b) Force actuator and collocated displacement transducer and (negative) lead controller (DVF is a particular case). (c) IFF control: root locus for a single mode.

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