Module 5: Principles of Active Vibration Control
  Lecture 28: Modelling of the Dynamic System
 

Modelling of the Dynamic System: (contd...)

If we assume velocity proportional control algorithm, the active strain becomes proportional to the transverse velocity of the beam , the symbol ‘.’ denotes differentiation with respect to time, the constant of proportionality C is function of electro/magneto-mechanical constant(d), and controller gain (f).

In the case of magnetostrictive material, , where the coil constant  is given by

(28.6)

where, nc is the total number of coil-turns, rc – effective length of magnetizing coil and wc – effective width of magnetizing coil.

Thus, stress at any layer may now be written as

)] (28.6)

Using the Hamilton's principle, the governing equations of motion may be derived as

) (28.7)

 

with the following boundary conditions:
i) either      or  
ii) either    or    
Initial conditions in time will also be prescribed along with.

Figure 28.3: Distributed control of a composite beam