Nonlinear control · Lablypedia

Control theory is divided into two branches. Linear control theory applies to systems made of devices which obey the superposition principle. They are governed by linear differential equations. A major subclass is systems which in addition have parameters which do not change with time, called linear time invariant (LTI) systems. These systems can be solved by powerful frequency domain mathematical techniques of great generality, such as the Laplace transform, Fourier transform, Z transform, Bode plot, root locus, and Nyquist stability criterion.

Nonlinear control theory covers a wider class of systems that do not obey the superposition principle. It applies to more real-world systems, because all real control systems are nonlinear. These systems are often governed by nonlinear differential equations. The mathematical techniques which have been developed to handle them are more rigorous and much less general, often applying only to narrow categories of systems. These include limit cycle theory, Poincaré maps, Lyapunov stability theory, and describing functions. If only solutions near a stable point are of interest, nonlinear systems can often be linearized by approximating them by a linear system obtained by expanding the nonlinear solution in a series, and then linear techniques can be used. Nonlinear systems are often analyzed using numerical methods on computers, for example by simulating their operation using a simulation language. Even if the plant is linear, a nonlinear controller can often have attractive features such as simpler implementation, faster speed, more accuracy, or reduced control energy, which justify the more difficult design procedure.

An example of a nonlinear control system is a thermostat-controlled heating system. A building heating system such as a furnace has a nonlinear response to changes in temperature; it is either "on" or "off", it does not have the fine control in response to temperature differences that a proportional (linear) device would have. Therefore, the furnace is off until the temperature falls below the "turn on" setpoint of the thermostat, when it turns on. Due to the heat added by the furnace, the temperature increases until it reaches the "turn off" setpoint of the thermostat, which turns the furnace off, and the cycle repeats. This cycling of the temperature about the desired temperature is called a limit cycle, and is characteristic of nonlinear control systems.

Properties of nonlinear systems

Some properties of nonlinear dynamic systems are

They do not follow the principle of superposition (linearity and homogeneity).
They may have multiple isolated equilibrium points.
They may exhibit properties such as limit cycle, bifurcation, chaos.
Finite escape time: Solutions of nonlinear systems may not exist for all times.

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Analysis and control of nonlinear systems

There are several well-developed techniques for analyzing nonlinear feedback systems:

Describing function method
Phase plane method
Lyapunov stability analysis
Singular perturbation method
The Popov criterion and the circle criterion for absolute stability
Center manifold theorem
Small-gain theorem
Passivity analysis

Control design techniques for nonlinear systems also exist. These can be subdivided into techniques which attempt to treat the system as a linear system in a limited range of operation and use (well-known) linear design techniques for each region:

Gain scheduling

Those that attempt to introduce auxiliary nonlinear feedback in such a way that the system can be treated as linear for purposes of control design:

Feedback linearization

And Lyapunov based methods:

Lyapunov redesign
Control-Lyapunov function
Nonlinear damping
Backstepping
Sliding mode control

Nonlinear feedback analysis – The Lur'e problem

An early nonlinear feedback system analysis problem was formulated by A. I. Lur'e. Control systems described by the Lur'e problem have a forward path that is linear and time-invariant, and a feedback path that contains a memory-less, possibly time-varying, static nonlinearity.

The linear part can be characterized by four matrices (A,B,C,D), while the nonlinear part is Φ(y) with $\frac{Φ (y)}{y} \in [a, b], a < b \forall y$ (a sector nonlinearity).

Absolute stability problem

Consider:

(A,B) is controllable and (C,A) is observable
two real numbers a, b with a < b, defining a sector for function Φ

The Lur'e problem (also known as the absolute stability problem) is to derive conditions involving only the transfer matrix H(s) and {a,b} such that x = 0 is a globally uniformly asymptotically stable equilibrium of the system.

There are two well-known wrong conjectures on the absolute stability problem:

The Aizerman's conjecture
The Kalman's conjecture.

Graphically, these conjectures can be interpreted in terms of graphical restrictions on the graph of Φ(y) x y or also on the graph of dΦ/dy x Φ/y. There are counterexamples to Aizerman's and Kalman's conjectures such that nonlinearity belongs to the sector of linear stability and unique stable equilibrium coexists with a stable periodic solution—hidden oscillation.

There are two main theorems concerning the Lur'e problem which give sufficient conditions for absolute stability:

The circle criterion (an extension of the Nyquist stability criterion for linear systems)
The Popov criterion.

Theoretical results in nonlinear control

Frobenius theorem

The Frobenius theorem is a deep result in differential geometry. When applied to nonlinear control, it says the following: Given a system of the form

\dot{x} = \sum_{i = 1}^{k} f_{i} (x) u_{i} (t)

where $x \in R^{n}$ , $f_{1}, \dots, f_{k}$ are vector fields belonging to a distribution $Δ$ and $u_{i} (t)$ are control functions, the integral curves of $x$ are restricted to a manifold of dimension $m$ if $span (Δ) = m$ and $Δ$ is an involutive distribution.