24.04.2013 Views

Nonlinear Control Sy.. - Free

Nonlinear Control Sy.. - Free

Nonlinear Control Sy.. - Free

SHOW MORE
SHOW LESS

Create successful ePaper yourself

Turn your PDF publications into a flip-book with our unique Google optimized e-Paper software.

20<br />

C T<br />

Figure 1.12: <strong>Nonlinear</strong> RLC-circuit.<br />

Figure 1.13: Unstable limit cycle.<br />

CHAPTER 1. INTRODUCTION<br />

Figure 1.13 shows the vector field diagram of this system with µ = 1. As can be seen in the<br />

figure, all trajectories diverge from the orbit and the limit cycle is unstable.<br />

1.8 Higher-Order <strong>Sy</strong>stems<br />

When the order of the state space realization is greater than or equal to 3, nothing<br />

significantly different happens with linear time-invariant systems. The solution of the state<br />

equation with initial condition x0 is still x = eATxo, and the eigenvalues of the A matrix<br />

still control the behavior of the trajectories. <strong>Nonlinear</strong> equations have much more room in<br />

which to maneuver. When the dimension of the state space realization increases from 2 to<br />

3 a new phenomenon is encountered; namely, chaos.

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!