Applied Mathematics and Mechanics (English Edition) ›› 2004, Vol. 25 ›› Issue (8): 854-862.

• Articles • Previous Articles     Next Articles

LINEAR ACTIVE STRUCTURES AND MODES(Ⅱ)—DISCRETE SYSTEMS AND BEAMS

WANG Yong-gang1,2, GONG Jing1,3, ZHANG Jing-hui1   

  1. 1. School of Civil Engineering and Mechanics, Xi’an Jiaotong University, Xi’an 710049, P. R. China;
    2. School of Science, Chang’an University, Xi’an 710064, P. R. China;
    3. Department of Civil Engineering, Northeast China Institute of Electric Power, Jilin 132012, P. R. China
  • Received:2002-11-01 Revised:2004-03-08 Online:2004-08-18 Published:2004-08-18
  • Supported by:

    the National Natural Science Foundation of China(10272087); the Associat-ed Foundation of the National Natural Science Foundation Committee of China and the Academy of Engi-neering Physics of China(10176042)

Abstract: The basic concepts about the active structures and some attributes of the modes were presented in paper “Liner Active Structures and Modes](I)". The characteristics of the active discrete systems and active beams were discussed, especially, the stability of the active structures and the orthogonality of the eigenvectors. The notes about modes were portrayed by a model of a seven-storeyed building with sensors and actuators. The concept of the adjoint active structure was extended from the discrete systems to the beams that were the representations of the continuous structures. Two types of beams with different placements of the measuring and actuating systems were discussed in detail. One is the beam with the discrete sensors and actuators, and the other is the beam with distributed sensor and actuator function. The orthogonality conditions were derived with the modal shapes of the active beam and its adjoint active beam. An example shows that the variation of eigenvalues with feedback amplitude for the homo-configuration and non-homo-configuration active structures.

Key words: active structures, beam, mode, orthogonal condition

2010 MSC Number: 

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