Negative imaginary systems

From testwiki
Jump to navigation Jump to search

Template:Multiple issues

Negative imaginary (NI) systems theory was introduced by Lanzon and Petersen in.[1][2] A generalization of the theory was presented in [3] In the single-input single-output (SISO) case, such systems are defined by considering the properties of the imaginary part of the frequency response G(jω) and require the system to have no poles in the right half plane and j(G(jω)G(jω)) > 0 for all ω in (0, ∞). This means that a system is Negative imaginary if it is both stable and a nyquist plot will have a phase lag between [-π 0] for all ω > 0.

Negative Imaginary Definition

Source:[3]

A square transfer function matrix G(s) is NI if the following conditions are satisfied:

  1. G(s) has no pole in Re[s]>0.
  2. For all ω0 such that jω is not a pole of G(s) and j(G(jω)G(jω))0.
  3. If s=jω0,ω0>0 is a pole of G(s), then it is a simple pole and furthermore, the residual matrix K=limsjω0(sjω0)jG(s) is Hermitian and positive semidefinite.
  4. If s=0 is a pole of G(s), then lims0skG(s)=0 for all k3 and lims0s2G(s) is Hermitian and positive semidefinite.

These conditions can be summarized as:

  1. The system G(s) is stable.
  2. For all positive frequencies, the nyquist diagram of the system response is between [-π 0].

Negative Imaginary Lemma

Source:[3]

Let [ABCD] be a minimal realization of the transfer function matrix G(s). Then, G(s) is NI if and only if D=DT and there exists a matrix

P=PT0, Wm×m,and Lm×n such that the following LMI is satisfied:

[PA+ATPPBATCTBTPCA(CB+BTCT)]=[LTLLTWWTLWTW]0.

This result comes from positive real theory after converting the negative imaginary system to a positive real system for analysis.

References

Template:Reflist