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Nonlinear Control Sy.. - Free

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1.9. EXAMPLES OF NONLINEAR SYSTEMS 23<br />

1.9.1 Magnetic Suspension <strong>Sy</strong>stem<br />

Figure 1.15: Magnetic suspension system.<br />

Magnetic suspension systems are a familiar setup that is receiving increasing attention in<br />

applications where it is essential to reduce friction force due to mechanical contact. Magnetic<br />

suspension systems are commonly encountered in high-speed trains and magnetic bearings,<br />

as well as in gyroscopes and accelerometers. The basic configuration is shown in Figure<br />

1.15.<br />

According to Newton's second law of forces, the equation of the motion of the ball is<br />

V (t)<br />

my = -fk + mg + F (1.27)<br />

where m is the mass of the ball, fk is the friction force, g the acceleration due to gravity,<br />

and F is the electromagnetic force due to the current i. To complete the model, we need to<br />

find a proper model for the magnetic force F. To this end we notice that the energy stored<br />

in the electromagnet is given by<br />

E = 1Li2<br />

where L is the inductance of the electromagnet. This parameter is not constant since it<br />

depends on the position of the ball. We can approximate L as follows:<br />

L = L(y) = 1+µy.<br />

(1.28)

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