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Yuri Shtessel Christopher Edwards Leonid Fridman - Sliding Mode Control and Observation

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Yuri Shtessel Christopher Edwards Leonid Fridman Sliding Mode Control and Observation

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Springer Science+Business Media New York 2014
Yuri Shtessel , Christopher Edwards , Leonid Fridman and Arie Levant Sliding Mode Control and Observation Control Engineering 10.1007/978-0-8176-4893-0_1
1. Introduction: Intuitive Theory of Sliding Mode Control
Yuri Shtessel 1, Christopher Edwards 2, Leonid Fridman 3 and Arie Levant 4
(1)
Department of Electrical and Computer Engineering, University of Alabama in Huntsville, Huntsville, AL, USA
(2)
College of Engineering, Mathematics and Physical Science, University of Exeter, Exeter, UK
(3)
Department of Control Division of Electrical Engineering, Faculty of Engineering National Autonomous University of Mexico, Federal District, Mexico
(4)
Department of Applied Mathematics School of Mathematical Sciences, Tel-Aviv University, Tel-Aviv, Israel
In the formulation of any practical control problem, there will always be a discrepancy between the actual plant and its mathematical model used for the controller design. These discrepancies (or mismatches) arise from unknown external disturbances, plant parameters, and parasitic/unmodeled dynamics. Designing control laws that provide the desired performance to the closed-loop system in the presence of these disturbances/uncertainties is a very challenging task for a control engineer. This has led to intense interest in the development of the so-called robust control methods which are supposed to solve this problem. One particular approach to robust controller design is the so-called sliding mode control technique.
In , the main concepts of sliding mode control will be introduced in an intuitive fashion, requiring only a basic knowledge of control systems. The sliding mode control design techniques are demonstrated on tutorial examples and via graphical exposition. Advanced sliding mode concepts, including sliding mode observers/differentiators and second-order sliding mode control, are studied at a tutorial level. The main advantages of sliding mode control, including robustness, finite-time convergence, and reduced-order compensated dynamics, are demonstrated on numerous examples and simulation plots.
For illustration purposes, the single-dimensional motion of a unit mass (Fig. ) is considered. A state-variable description is easily obtained by introducing variables for the position and the velocity Sliding Mode Control and Observation - image 1 so that
11 where u is the control force and the disturbance term f x 1 x 2 t - photo 2
(1.1)
where u is the control force, and the disturbance term f ( x 1, x 2, t ), which may comprise dry and viscous friction as well as any other unknown resistance forces, is assumed to be bounded, i.e., f ( x 1, x 2, t ) L > 0. The problem is to design a feedback control law u = u ( x 1, x 2) that drives the mass to the origin asymptotically. In other words, the control u = u ( x 1, x 2) is supposed to drive the state variables to zero: i.e., Sliding Mode Control and Observation - image 3 . This apparently simple control problem is a challenging one, since asymptotic convergence is to be achieved in the presence of the unknown bounded disturbance f ( x 1, x 2, t ). For instance, a linear state-feedback control law
12 provides asymptotic stability of the origin only for f x 1 x 2 t 0 - photo 4
(1.2)
provides asymptotic stability of the origin only for f ( x 1, x 2, t ) 0 and typically only drives the states to a bounded domain ( k 1, k 2, L ) for f ( x 1, x 2, t ) L > 0.
Fig 11 Single-dimensional motion of a unit mass Example 11 The results - photo 5
Fig. 1.1
Single-dimensional motion of a unit mass
Example 1.1.
The results of the simulation of the system in Eqs. (.
Fig 12 Asymptotic convergence for f x 1 x 2 t 0 Fig 13 - photo 6
Fig. 1.2
Asymptotic convergence for f ( x 1, x 2, t ) 0
Fig 13 Convergence to the domain for f x 1 x 2 t sin2 t The - photo 7
Fig. 1.3
Convergence to the domain for f ( x 1, x 2, t ) = sin(2 t )
The question is whether the formulated control problem can be addressed using only knowledge of the bounds on the unknown disturbance.
1.1 Main Concepts of Sliding Mode Control
Let us introduce desired compensated dynamics for system (). A good candidate for these dynamics is the homogeneous linear time-invariant differential equation:
Sliding Mode Control and Observation - image 8
(1.3)
Since Sliding Mode Control and Observation - image 9 , a general solution of Eq. () and its derivative is given by
14 both x 1 t and x 2 t converge to zero asymptotically Note no - photo 10
(1.4)
both x 1( t ) and x 2( t ) converge to zero asymptotically. Note, no effect of the disturbance f ( x 1, x 2, t ) on the state compensated dynamics is observed. How could these compensated dynamics be achieved? First, we introduce a new variable in the state space of the system in Eq. ():
Sliding Mode Control and Observation - image 11
(1.5)
In order to achieve asymptotic convergence of the state variables x 1, x 2 to zero, i.e., Sliding Mode Control and Observation - image 12 , with a given convergence rate as in Eq. ():
Sliding Mode Control and Observation - image 13
(1.6)
For the -dynamics () a candidate Lyapunov function (see Appendix D) is introduced taking the form
Sliding Mode Control and Observation - image 14
(1.7)
In order to provide the asymptotic stability of Eq. () about the equilibrium point = 0, the following conditions must be satisfied:
(a)
Sliding Mode Control and Observation - image 15 for 0
(b)
Sliding Mode Control and Observation - image 16
Condition (b) is obviously satisfied by V in Eq. (). In order to achieve finite-time convergence (global finite-time stability), condition (a) can be modified to be
Sliding Mode Control and Observation - image 17
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