Non-uniform stabilization of control systems

Size: px
Start display at page:

Download "Non-uniform stabilization of control systems"

Transcription

1 IMA Journal of Mathematical Control and Information 2002) 19, Non-uniform stabilization of control systems IASSON KARAFYLLIS Department of Mathematics, National Technical University of Athens, Zografou Campus, 15780, Athens, Greece [Received on 10 March 2002; accepted on 6 June 2002] A version of non-uniform in time robust global asymptotic stability is proposed and enables us to derive: 1) sufficient conditions for the stabilization of uncertain nonlinear triangular time-varying control systems; 2) sufficient conditions for the solution of the partial-state global stabilization problem for autonomous systems. The results are obtained via the method of integrator backstepping and are generalizations of the existing corresponding results in the literature. Keywords: integrator backstepping; time-varying feedback; time-varying systems. 1. Introduction The notion of non-uniform in time Robust Global Asymptotic Stability RGAS) has been proved to be fruitful for the solution of several problems in Control Theory see Karafyllis & Tsinias, 2002a,b; Tsinias & Karafyllis, 1999; Tsinias, 2000) for applications to tracking problems and to the robust stabilization of uncertain systems that cannot be stabilized by continuous static time-invariant feedback and Karafyllis & Tsinias, 2001) for the extension of the notion of Input-to-State Stability ISS) to the time-varying case). It is shown in Karafyllis & Tsinias 2001, 2002b) that, even for autonomous systems for which uniform in time asymptotic stabilization by a continuous static feedback is not feasible, it is possible to exhibit non-uniform in time asymptotic stabilization by means of a smooth time-varying feedback. In this paper our interest is focused on uncertain nonlinear time-varying triangular systems. In order to find sufficient conditions for the robust stabilization of such systems, we first strengthen the notion of Robust Global Asymptotic Stability RGAS) given in Karafyllis & Tsinias 2001), by introducing the notion of φ-rgas in such a way that it allows the estimation of the rate of convergence to the equilibrium point. Roughly speaking, for the system ẋ = f t, x, d) x R n, t 0, d D 1.1) where D R m is a compact set and f t, 0, d) = 0 for all t, d) R + D, wesay that 0 R n is φ-rgas if it is in general non-uniformly in time RGAS and particularly, there exists a smooth function φ :R + [1, + ) such that every solution of 1.1) satisfies the following property: lim t + φ p t) xt) =0, p 0 1.2) c The Institute of Mathematics and its Applications 2002

2 420 I. KARAFYLLIS In Section 3 we develop the main tool for the integrator backstepping method that it is used in this paper, and in Section 4 this tool is used for the following triangular system: ẋ i = f i t,θ,x 1,...,x i ) + g i t,θ,x 1,...,x i )x i+1 i = 1,...,n u := x n+1 1.3) x = x 1,...,x n ) T R n, t 0, u R where the uncertainty θ = θt) is any measurable function taking values in a compact set Ω R l.weobtain a set of sufficient conditions Proposition 4.1) for the robust global asymptotic stabilization of 1.3), which is a direct generalization of the corresponding set of sufficient conditions given in the literature for the autonomous case Jiang et al., 1994; Tsinias, 1996). The problem of the stabilization by means of partial-state time-varying feedback is also addressed Proposition 4.2). Specifically, we study systems of the form ż = f 0 t,θ,z, x 1 ) ẋ i = f i t,θ,z, x 1,...,x i ) + g i t,θ,z, x 1,...,x i )x i+1 i = 1,...,n 1.4) u := x n+1 where z R m, x = x 1,...,x n ) T R n, u R, θ = θt) is any measurable function taking values in a compact set Ω R l, and we obtain sufficient conditions for the robust global asymptotic stabilization of 1.4) by means of a partial state smooth time-varying feedback of the form u = kt, x). Using these results, we next study the applications of time-varying feedback to autonomous control systems. In Section 5, the following two applications of time-varying feedback to autonomous control systems are studied: 1) We prove that for every function φ ) there exists a smooth time-varying feedback of the form u = kt, x),such that 0 R n is φ-rgas for the system ẋ i = f i θ, x 1,...,x i ) + g i θ, x 1,...,x i )x i+1 i = 1,...,n 1.5) u := x n+1 where x = x 1,...,x n ) T R n, u R, θ = θt) is any measurable function taking values in a compact set Ω R l Corollary 5.1). Roughly speaking, this means that we can design a smooth time-varying feedback so that the solutions of 1.5) converge to the equilibrium point as fast as desired. We emphasize that this feature cannot be accomplished by the use of locally Lipschitz time-invariant feedback. 2) The stabilization of autonomous systems by means of partial-state smooth timevarying feedback Theorem 5.4). Specifically, consider the system ż = f 0 z, x, u) 1.6a) ẋ i = f i θ, x 1,...,x i ) + g i θ, x 1,...,x i )x i+1 i = 1,...,n u := x n+1 1.6b) where z R m, x = x 1,...,x n ) T R n, u R, θ = θt) is any measurable function taking values in a compact set Ω R l, f 0, f i and g i are continuous with respect to θ Ω and locally Lipschitz with respect to z, x, u), uniformly in θ Ω, with f 0 0, 0, 0) = 0, f i θ, 0,...,0) = 0 for all θ Ω, for i = 1,...,n.

3 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 421 System 1.6) can be regarded as the cascade connection of two subsystems. Sufficient conditions for the global asymptotic stability of the equilibrium point for a cascade connection of two independent subsystems were given in Jiang et al. 1994) and recently in Panteley & Loria 1998). We provide sufficient conditions for the existence of a smooth partial-state time-varying feedback of the form u = kt, x), such that 0 R m R n is GAS. This is achieved in Theorem 5.4 and to this end we are using the Lyapunov characterization of forward completeness given in Angeli & Sontag 1999). We guarantee the existence of such a feedback, under the hypotheses: i) Subsystem 1.6a) is forward complete with x, u) as input. ii) 0 R m is GAS for the unforced subsystem ż = f 0 z, 0, 0) 0-GAS property). This is a generalization of the existing results since forward completeness and 0-GAS is weaker than ISS or even iiss as shown in Angeli et al., 2000). Notation * By C j A)C j A; Ω)), where j 0isanon-negative integer, we denote the class of functions taking values in Ω) that have continuous derivatives of order j on A. * By B r B r ), where r > 0, we denote the open closed) ball of radius r in R n, centred at 0 R n. * For definitions of classes K, K, KL see [8]. * By D + f t) we denote the upper right-hand side Dini derivative of the scalar function f, i.e. D + f t+h) f t) f t) = lim sup h 0 + h. * We denote by M D the class of measurable functions d :R + D. 2. Definitions and preliminary technical results In this section we give the notion of φ-rgas for time-varying systems and we present definitions and technical lemmas that play a key role in proving the main results of the paper. Their proofs can be found in the Appendix. DEFINITION 2.1 We denote by K + the class of non-decreasing C functions φ :R + R with φ0) 1, and we denote by K K +, the class of C functions that belong to K + φt) and satisfy lim t + φ r t) = 0, for some r 1. For example the functions φt) = 1, φt) = 1 + t, φt) = expt) all belong to the class K. The following lemma states some of the properties of these classes of functions. LEMMA 2.2 For every p K, q K and for all constants M 1 and a 0, it holds that the functions p )+q ), p )q ) and Mp a ) are of class K as well. Furthermore, for every function φ of class K +, there exists a function φ of class K,such that φt) φt) for all t 0. We next give the notion of φ-rgas, which directly extends the notion of RGAS presented in Karafyllis & Tsinias 2001). This notion is introduced in such a manner that we can have an estimate of the rate of convergence of the solution to the equilibrium point. Consider the system 1.1), where D is a compact subset of R m and the vector field f :R + R n D R n satisfies the following conditions:

4 422 I. KARAFYLLIS 1) The function f t, x, d) is measurable in t, for all x, d) R n D. 2) The function f t, x, d) is continuous in d, for all t, x) R + R n. 3) The function f t, x, d) is locally Lipschitz with respect to x, uniformly in d D, in the sense that for every bounded interval I R + and for every compact subset S of R n, there exists a constant L 0 such that f t, x, d) f t, y, d) L x y t I, x, y) S S, d D 2.1) with f t, 0, d) = 0, for all t, d) R + D. Let us denote by xt, t 0, x 0 ; d) = xt) the unique solution of 1.1) at time t that corresponds to input d M D with initial condition xt 0 ) = x 0 see Fillipov, 1988). DEFINITION 2.3 Let φ be a function of the class K +. We say that 0 R n is φ-robustly Globally Stable φ-rgs), if for every T 0, p 0 and ε>0, it holds that sup{φ p t) xt) :d M D, t t 0, x 0 ε, t 0 [0, T ]} < + and there exists a δ = δε, T, p) >0such that φ p t) xt) ε, for all x 0 δ, t t 0, t 0 [0, T ] and input d M D. 0 R n is called a φ-robust Global Attractor φ-rga), if for every R > 0, ε>0, p 0 and T 0, there is a τ := τε,t, R, p) 0 such that φ p t) xt) ε for all x 0 B R, t t 0 + τ, t 0 [0, T ] and input d M D. 0 R n is called φ-robustly Globally Asymptotically Stable φ-rgas), if it is φ-rgs and φ-rga. If 0 R n is φ-rgas for φt) := 1 then we simply write that 0 R n is RGAS. In Tsinias & Karafyllis 1999) we required t N xt) ε for every integer N 0in the definition of the L t Global Asymptotic Stability. It is clear that the present definition includes this case with φt) = 1+t K. The following lemma clarifies the consequences of the notion of φ-rgas and provides estimates of the solutions. LEMMA 2.4 Suppose that 0 R n is φ-rgas, for system 1.1) with d D as input. Then the following statements hold: i) For every function φ K + that satisfies φt) φt) for all t 0, 0 R n is φ-rgas for system 1.1). Particularly, 0 R n is RGAS. ii) For every pair of constants R 1 and p 0, 0 R n is φ-rgas, for system 1.1), where φt) = Rφ p t). iii) For every p 0, there exist functions σ ) KL and β ) K +, such that the following estimate holds for the solution of 1.1): xt) 1 φ p t) σ βt 0) x 0, t t 0 ), t t 0, d M D. 2.2) For the construction of a smooth time-varying feedback, we need to introduce the following class of convex functions. DEFINITION 2.5 We say that a :R + R + belongs to K con if:

5 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 423 1) a C 1 R + ) K. 2) The function da ds s) is non-decreasing. The following technical lemmas state some important properties of class K con that are used in the subsequent sections of this paper. LEMMA 2.6 The following statements hold: i) K con K. ii) If a,β belong to K con then a + β,aβ,aoβ also belong to K con. iii) For every a C 0 R + ) there exists a constant R > 0 and a function β K con such that as) R + βs), s 0. iv) If a ) K con the following properties hold: λas) aλs), s 0, λ 1 2.3a) as 1 ) + as 2 ) as 1 + s 2 ) a2s 1 ) + a2s 2 ), s 1, s 2 ) R +) b) LEMMA 2.7 Consider the vector field f C 0 Ω R n ;R m ), where Ω R l is a compact set, which is locally Lipschitz with respect to x R n, uniformly with respect to θ Ω and satisfies f θ, 0) = 0, for all θ Ω. Then there exists a K con such that: f θ, x) a x ), θ, x) Ω R n. 2.4) LEMMA 2.8 For every a K con, there exists an odd function β C R), functions γ K con, ã K con C R + ) and a constant R > 0, with the following properties: as) ãs), s 0 2.5) as) βs) γs), s 0 2.6) dβ ds s) R + γs), s ) The next lemma shows a fundamental property of forward complete time-varying systems. It shows that the reachable set contains a closed ball of positive radius at all times. This fact is going to be used in Section 3 of the paper. LEMMA 2.9 Consider system 1.1) and suppose that there exists a function ρ ) K con and a function φ ) K + such that f t, x, d) ρφt) x ), t, x, d) R + R n D. 2.8) Suppose, furthermore, that for all r 0, t 0 0 and t t 0 we have sup { xt) ; x 0 r, d M D } < ) Then it holds that B βt,t0,r) {xt); x 0 r, d M D } 2.10) where βt, t 0, r) is the unique solution of initial value problem: ẇ = ρφt)w) w R,wt 0 ) = r )

6 424 I. KARAFYLLIS 3. Adding a time-varying integrator The following technical lemma is the basic tool in the integrator backstepping method that we intend to use. Notice that in the time-varying case, there are many technical difficulties to obtain such a result, concerning the rate of convergence of the solution to the equilibrium point, as well as the issue of whether the dynamics converge to zero or not. Most of the technical assumptions introduced below are automatically satisfied in the autonomous case. LEMMA 3.1 Consider the system ẋ = Ft,θ,x, y) ẏ = f t,θ,x, y) + gt,θ,x, y)u x R n, y R, u R, t 0,θ Ω 3.1a) 3.1b) where Ω R l is a compact set, with Ft,θ,0, 0) = 0, f t,θ,0, 0) = 0, for all t,θ) R + Ω and F, f, g are measurable with respect to t, continuous with respect to θ, and locally Lipschitz with respect to x, y) uniformly in θ Ω. Suppose that there exists φ K such that the following hold: H1) There exists a function γ K, being locally Lipschitz on R +,ac j j 1) mapping k :R + R n Rwith k, 0) = 0, a constant µ 0, such that 0 R n is φ-rgas for ẋ = F t,θ,x, kt, x) + d γ x ) ) φ µ 3.2) t) with θ, d) D := Ω [ 1, 1] as input. H2) There exists a function p K con such that s pγ s)), s ) H3) There exists a K con such that the following inequalities hold for all t,θ,x, y) R + Ω R n R: Ft,θ,x, y) aφt) x, y) 3.4) kt, x) + k t, x) t aφt) x ) 3.5) k t, x) t φt) + aφt) x ). 3.6) H4) There exist constants K > 0andδ 0 such that the following inequalities hold for all t,θ,x, y) R + Ω R n R: 1 K φ δ gt,θ,x, y) φt) + aφt) x, y) ) 3.7) t) f t,θ,x, y) aφt) x, y) ). 3.8)

7 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 425 Then for every locally Lipschitz function Γ ) K, there exists a C mapping k : R + R Rwith k, 0) = 0 and constants M 1, q 1, such that 0 R n+1 is φ-rgas for d dt x = Ft,θ, x, kt, y kt, x)) + dγ x )) 3.9) with θ, d) D := Ω [ 1, ) 1] as input, where x := x, y), Ft, θ, x, u) := Ft,θ,x, y) and f t,θ,x, y) + gt,θ,x, y)u φt) := Mφ q t). 3.10) Furthermore, there exists a function ã ) K con,such that hypothesis H3) is satisfied with F ), x, kt, x) := kt, y kt, x)), ã ) and φ ) instead of F ), x, kt, x), a ) and φ ), respectively. When φ ) is bounded then the mapping k can be chosen to be independent of t. Proof. Let Φt, t 0, x 0 ; θ, d)) denote the solution of 3.2) initiated from x 0 R n at time t 0 0 and corresponding to input θ, d) M D and xt) = xt), yt)) denote the solution of 3.9) initiated from x 0 R n+1 at time t 0 0 and corresponding to input θ, d) M D. The proof is based on the following observations: i) By property ii) of Lemma 2.4 and definition 3.10), it suffices to show that 0 R n+1 is φ-rgas for 3.9) with θ, d) D := Ω [ 1, 1] as input. ii) In order to prove that 0 R n+1 is φ-rgas for 3.9) with θ, d) D := Ω [ 1, 1] as input, it suffices to show that there exists a function G ) K con and a C 0 function E :R + R + R + with Et, ) K for all t 0 and E, s) being non-decreasing, in such a way that the following inequality holds for all t t 0, s 0: sup{ xt) ; x 0 s,θ,d) M D } 3.11) Gφt) sup{ Φt, t 0, x 0 ; θ, d)) ; x 0 Et 0, s), θ, d) M D }). Indeed, notice that by virtue of 3.11), property iv) of Lemma 2.6 and the facts that φt) 1 and E, s) is non-decreasing, we have for all q 0, T 0, s 0 and h 0: sup {φ q t 0 + h) xt 0 + h) ; x 0 s, t 0 [0, T ],θ,d) M D } G φ q+1 t 0 + h) sup { Φt 0 + h, t 0, x 0 ; θ, d)) ; x 0 ET, s), t 0 [0, T ],θ,d) M D } ). 3.12) Furthermore, by virtue of iii) of Lemma 2.4 and the fact that 0 R n is φ-rgas for 3.2), it follows that there exist functions σ ) KL and β ) K +, such that the following estimate holds for the solution of 3.2): φ q+1 t) Φt, t 0, x 0 ; θ, d)) σ βt 0 ) x 0, t t 0 ), t t 0, θ, d) M D. 3.13) Combining 3.12) with 3.13) we obtain the following estimate, which holds for all h, s, T, q 0: sup { φ q t 0 + h) xt 0 + h) ; x 0 s, t 0 [0, T ],θ,d) M D } G σβt )ET, s), h)),

8 426 I. KARAFYLLIS which implies that 0 R n+1 is φ-rgas for 3.9) with θ, d) D := Ω [ 1, 1] as input. Since the proof is long and technical, we divide it into two parts. First part: Construction of Feedback. Given a locally Lipschitz function Γ ) K,we construct the feedback law kt, x) := kt, y kt, x)), where k ) C R + R) with k, 0) = 0, such that the analogue of H3) is satisfied. Second part: Stability Analysis. Exploiting the properties of the constructed feedback and Lemma 2.9, we prove that 3.11) holds for appropriate functions G ) K con and a E ) C 0 R + R + ). The methodology used is entirely different from the methodology used in Tsinias & Karafyllis 1999) for the case φt) = 1 + t. Without loss of generality, we may assume that the function p ), involved in 3.3), is of class K con C R + ). Indeed, this follows from Lemma 2.8, which guarantees the existence of a function p ) K con C R + ) that satisfies ps) ps), for all s 0. Consequently, if p ) is not of class K con C R + ),wecan replace it by p ). Similarly, without loss of generality, we may assume that γ K con C R + ), because if this is not the case then we can replacep ) K con C R + ) in 3.3) by ps) := ps) + s and γs) by γs) := p 1 s) γs), which belongs to K C R + ). First part: Construction of Feedback. In this part of proof we use repeatedly inequalities 2.3a), 2.3b) of Lemma 2.6 for functions of class K con,aswell as the fact that φt) 1 for all t 0. Notice that, by application of Lemma 2.7, to the even extensions of γ and Γ ) which are locally Lipschitz), there exist functions γ ) K con and Γ ) K con such that γs) γs), s a) Γ s) Γ s), s b) Define u := kt, z) + dγ x ) 3.15a) z := y kt, x) 3.15b) where k ) is yet to be selected. We get from 3.1) and 3.15a), 3.15b): ż = f t,θ,x, kt, x) + z) + dgt,θ,x, kt, x) + z)γ x ) k t, x) t k 3.15c) t, x)ft,θ,x, kt, x) + z) + gt,θ,x, kt, x) + z)kt, z). t

9 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 427 Moreover, by 3.3), 3.5), 3.14a) and 3.15b), there exist functions G i ) K con i = 1,...,3) such that ) x G 1 φ µ+1 t) z, when γ x ) 2φ µ t) z 3.16a) x G 2 φt) x ), when φ µ t) z γ x ) 3.16b) z G 3 φt) x ), t, x) R + R n c) where µ 0isthe constant involved in 3.2). Furthermore, property iii) of Lemma 2.6 implies the existence of a function G 4 ) K con and a constant R 1 > 0 such that { } dγ 0 max 0 ξ s ds ξ) R 1 + G 4 s), s d) It follows from 3.4), 3.5), 3.6), 3.7), 3.8), 3.14b), 3.15c), 3.16a) and 3.16d) that there exists a constant ν 2 and functions a i ) K con, i = 1, 2, that satisfy the following inequalities: d dt zt) a 1φ µ+ν t) z ) + sgnz)gt,θ,x, kt, x) + z)kt, z), for 2φ µ t) z γ x ) and z = ) d dt γ xt) ) a 2φ µ+ν t) z ), for 2φ µ t) z γ x ) >0 3.18) Since φ K, there exist constants K 0 and r 1 with 0 φt) K φ r t), t ) Inequalities 3.17), 3.18) in conjunction with 3.19) imply d φ µ t) zt) γ xt) ) ) K µφ σ t) z +a 1 φ σ t) z ) + a 2 φ σ t) z ) dt + φ µ t)sgnz)gt,θ,x, kt, x) + z)kt, z) for 2φ µ t) z γ x ) >0 3.20a) where d φ µ t) zt) ) K µφ σ t) z +a 1 φ σ t) z ) dt + φ µ t)sgnz)gt,θ,x, kt, x) + z)kt, z) for 2φ µ t) z γ x ) and z = b) We define the function a 3 ) K con : σ := 2µ + ν + r ) a 3 s) := a 1 s) + a 2 s) + K µs + R 1 + G 4 s))ρs) 3.22)

10 428 I. KARAFYLLIS ρs) := a s + as) + γs)) 3.23) where γ ) K con, R 1 > 0 and G 4 ) K con are defined in 3.14a) and 3.16d), respectively. Notice that, by virtue of 3.4), 3.5), 3.14a) and definition 3.23), we have F t,θ,x, kt, x) + d γ x ) ) φ µ ρφ 2 t) x ). 3.24) t) Furthermore, by virtue of Lemma 2.8, there exists an odd C function ψ ), afunction G 5 ) K con and a constant R 2 > 0, with the following properties: a 3 s) ψs) G 5 s), s 0 dψ ds s) R 2 + G 5 s), s a) 3.25b) We also define kt, z) := ψ 1 + K )φ σ +δ t)z ) 3.26) where K > 0 and δ 0 are the constants involved in 3.7). It is clear that the mapping kt, x, y) = kt, y kt, x)) is of class C j R + R n+1 ).Moreover, inequalities 3.5), 3.6), 3.19) in conjunction with 3.25a), 3.25b) imply that there exists a function ã ) K con and constants q 1, M 1, such that H3) is satisfied with x, k ), ã ) and φ ) instead of x, k ), a ) and φ ), respectively, where φ ) is defined in 3.10) and is of class K by virtue of iii) of Lemma 2.2. When φ ) is bounded we may select for R := sup t 0 φt): kt, z) := kz) = ψ ) 1 + K ) R σ +δ z ) The major property of the constructed feedback is the following inequality, which is a consequence of 3.7), 3.16d), 3.22), 3.25a), 3.26) and the fact that the function ψ ) is odd: sgnz)φ µ t)gt,θ,x, kt, x) + z)kt, z) K µφ σ t) z a 1 φ σ t) z ) a 2 φ σ t) z ) dγ φ µ t) z ) ) ρ φ 2+µ t) z. 3.27) ds Notice that by virtue of inequalities 3.20a), 3.20b) and 3.27), it follows that: d φ µ t) zt) γ xt) ) ) 0, when 2φ µ t) z γ x ) >0 3.28a) dt d dt φ µ t) zt) ) dγ ds φ µ t) z ) ρ φ 2+µ t) z ), when 2φ µ t) z γ x ) and z = b)

11 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 429 Second part: Stability Analysis. We define: L t := { x, y) R n R:φ µ t) y kt, x) γ x ) }. 3.29) Notice that by virtue of 3.28a) and definitions 3.15b), 3.29) of z, L t, respectively, it follows that the region L t is positively invariant the case x =0implies z = 0, which is the equilibrium position of 3.9)). As long as the trajectory of the solution of 3.9) remains outside L t we obtain using 3.15b), 3.28b) and 3.29) that D + φ µ t) zt) ) dγ ) ds φµ t) zt) )ρ φ 2+µ t) zt). 3.30) Let βt, t 0, r) denote the unique solution of the following initial value problem: ẇ = ρ φ 2 t)w ) w R,wt 0 ) = r 0. Indeed, by virtue of inequality 3.24) and Lemma 2.9, we guarantee that 3.31) B βt,t0,r) {Φt, t 0, x 0 ; θ, d)), x 0 r,θ,d) M D } 3.32) where Φt, t 0, x 0 ; θ, d)) denotes the solution of 3.2) initiated from x 0 R n at time t 0 0 and corresponding to input θ, d) M D. Furthermore, differential inequality 3.30) implies by virtue of the comparison principle in Khalil, 1996): φ µ t) zt) γβt, t 0,γ 1 φ µ t 0 ) zt 0 ) ))) as long as the trajectory of 3.9) remains outside L t. 3.33) Thus by 3.14a), 3.16a), 3.16c) and 3.33) we obtain the estimate for the solution of 3.9): xt) G 1 φt) γ βt, t0,γ 1 φ µ t 0 )G 3 φt 0 ) xt 0 ) ))) )) as long as the trajectory of 3.9) remains outside L t. 3.34) Moreover, by virtue of 3.32), 3.33) and the facts that G 3 ), γ ) K con, φt) 1 and using property iv) of Lemma 2.6, we obtain that the following estimate holds for G 6 := G 1 o γ : sup { xt) ; x 0 s,θ,d) M D } { G 6 φt) ) }) sup Φt, t 0, x 0 ; θ, d)) ; x 0 γ 1 G 3 φ µ+1 t 0 )s),θ,d) M D as long as the trajectory of 3.9) remains outside L t. 3.35) Let us denote by T + the first time that the solution is entering L T. Notice that for all t T,bypositive invariance of L t, the solution remains inside L t. Moreover, there exists an input θ, d) M D such that component xt) of the solution xt) of 3.9) satisfies xt) Φt, T, xt ); θ, d)), for all t T. Let t t 0 be arbitrary. We distinguish the cases:

12 430 I. KARAFYLLIS a) T = t 0.Inthis case we have xt) sup{ Φt, t 0, x 0 ; θ, d)) ; θ, d) M D } and consequently using 3.16b) we obtain the estimate: sup { xt) ; x 0 s,θ,d) M D } 3.36) G 2 φt) sup { Φt, t 0, x 0 ; θ, d)) ; x 0 s,θ,d) M D }). b) T / [t 0, t].inthis case estimate 3.35) holds. c) t 0 < T t.inthis case we have: xt) sup { Φt, T, xt ); θ, d)) ; T [t 0, t],θ,d) M D } By definition 3.29) and continuity of the solution we also have for the case c): γ xt ) ) = φ µ T ) zt ). Moreover, estimate 3.33) implies φ µ T ) zt ) γβt, t 0,γ 1 φ µ t 0 ) z 0 ))). These estimates in conjunction with 3.16b), 3.16c) give sup { xt) ; x 0 s,θ,d) M D } G 2 φt) sup I ) 3.37a) { I := Φt, T, xt ); θ, d)) ; T [t 0, t],θ,d) M D, xt ) β T, t 0,γ 1 φ µ t 0 )G 3 φt 0 )s) ))}. 3.37b) Inclusion 3.32) in conjunction with estimate 3.37) and the fact that G 3 ) K con and φt) 1, shows that the following estimate holds for case c): sup { xt) ; x 0 { s,θ,d) M D } G 2 φt) sup Φt, t0, x 0 ; θ, d)) ; x 0 γ 1 G 3 φ µ+1 t 0 )s) ) }),θ,d) M D. 3.38) Combining estimates 3.35), 3.36) and 3.38) for the cases a), b) and c), respectively, we obtain the desired inequality 3.11) for Gs) := 2G 2 s) + G 6 s) 3.39a) { } Et 0, s) := max s,γ 1 G 3 φ µ+1 t 0 )s)). 3.39b) Indeed, by virtue of property ii) of Lemma 2.6, we have G ) K con. The proof is complete. The following lemma provides a sufficient condition for hypothesis H2). In fact, Lemma 3.2 shows that hypothesis H2) is the analogue of the hypothesis of local exponential stability made in Jiang et al. 1994), Tsinias 1996) for the autonomous case. LEMMA 3.2 Suppose that γ K is a locally Lipschitz function that satisfies γs) Λs, s [0,η], for some constants η, Λ > 0. Then H2) is satisfied. Proof. Clearly, γ 1 s) Λ 1 s, for all s [0,γη)] and consequently the function γ gs) := sup 1 u) 0<u s u is continuous on 0, + ), positive and non-decreasing with gs) Λ 1 for all s 0,γη)]. Defining g0) := lim s 0 + gs), wehaveγ 1 s) gs)s, forall s 0. We also define hs) := s+1 0 gr)dr, which satisfies hs) gs), for all s 0and notice that the function ps) := hs)s is of class K con. Combining, we get γ 1 s) ps), for all s 0, which implies H2).

13 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS Applications to time-varying control systems We are now ready to apply induction using Lemma 3.1 and the method of integrator backstepping for the stabilization of system 1.3). PROPOSITION 4.1 Consider system 1.3), where x = x 1,...x n ) T R n, θ Ω R l, Ω being a compact set, f i and g i are measurable with respect to t 0, continuous with respect to θ Ω and locally Lipschitz with respect to x 1,...x i ), uniformly in θ Ω, for i = 1,...,n. Suppose that there exist functions φ K, a K con, constants δ 0, K > 0, such that the following hold for all t, x,θ) R + R n Ω and i = 1,...,n: f i t,θ,x 1,...,x i ) aφt) x 1,...,x i ) ) 4.1) 1 K φ δ t) g it,θ,x 1,...,x i ) φt) + aφt) x 1,...,x i ) ). 4.2) Then for every locally Lipschitz function Γ ) K there exists a C mapping k : R + R n Rwith k, 0) = 0, a function η K con and a constant p 0, with kt, x) η φ p t) x ), t, x) R + R n 4.3) such that 0 R n is φ-rgas for the following system: ẋ i = f i t,θ,x 1,...,x i ) + g i t,θ,x 1,...,x i )x i+1 i = 1,...,n x n+1 = kt, x) + dγ x ) 4.4) with θ, d) D := Ω [ 1, 1] as input. Moreover, when φ ) is bounded then the mapping k can be chosen to be independent of t. Proof. The proof of the general case is based on Lemma 3.1 and follows by using standard induction arguments like those given in Jiang et al. 1994). For reasons of simplicity we consider the case n = 2. The general case follows similarly by induction. First we consider the one-dimensional subsystem ẋ 1 = f 1 t,θ,x 1 ) + g 1 t,θ,x 1 )x 2 with x 2 as input. 4.5) Let M > 0. We define ãs) := 1 + s)as) M)s 4.6) which obviously by Lemma 2.6 is of class K con.bylemma 2.8 there exists an odd function ψ ) C R),afunction β ) K con and a constant R 1 > 0 such that ãs) ψs) βs), s 0 dψ ds s) R 1 + βs), s a) 4.7b)

14 432 I. KARAFYLLIS Furthermore, since φ ) K, there exists a constant r 1 such that lim t + φt) φ r t) = c) We set k 1 t, x 1 ) := ψ1 + K )φ 1+δ+r t)x 1 ) 4.8) or for the case of bounded φ ) K with R 2 := sup t 0 φt): k 1 t, x 1 ) := k 1 x 1 ) = ψ1 + K )R 1+r+δ 2 x 1 ) 4.8 ) where K,δ are the constants involved in 4.2). Obviously k 1 ) is a function of class C R + R) with k 1, 0) = 0. It follows from 4.2), 4.6), 4.7a) and definition 4.8), the fact that ψ ) is odd and φt) 1 for all t 0, as well as iv) of Lemma 2.6, that the following inequality holds for all t,θ,x 1 ) R + Ω R: ) sgnx 1 )g 1 t,θ,x 1 )k 1 t, x 1 ) ã φ r+1 t) x 1 Mφ r t) x x 1 )aφt) x 1 ) φt) x ) Moreover, inequalities 4.7a) 4.7c) and definition 4.8) imply the existence of constants R 3 1, σ 1 and a function ζ ) K con,such that the following inequalities hold for all t, x 1 ) R + R: k 1 t, x 1 ) + k 1 t t, x ) 1) ζ φt) x a) k 1 t, x 1 ) x φt) + ζ φt) x 1 ) b) φt) := R 3 φ σ t). 4.10c) We claim that 0 Ris φ-rgas for the closed-loop system 4.5) with x 2 = k 1 t, x 1 ) + d x 1, d [ 1, 1]. Inorder to prove this claim, notice that by 4.1), 4.2) and 4.9) we have for all x 1 = 0, t 0 and θ, d) D = Ω [ 1, 1]: d dt x 1 =sgnx 1 ) f t,θ,x 1 ) + sgnx 1 )gt,θ,x 1 )k 1 t, x 1 ) + sgnx 1 )gt,θ,x 1 )d x 1 Mφ r t) x 1. Since x 1 = 0isthe equilibrium point of the closed-loop system 4.5) with x 2 = k 1 t, x 1 )+ d x 1, d [ 1, 1] we get D + x 1 t) Mφ r t) x 1 t), for all t t )

15 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 433 The differential inequality 4.11) and the comparison lemma in Khalil 1996) give for all q 0, s 0: sup { φ q } t t) x 1 t) ; x 1 t 0 ) s,θ,d) M D φ q t 0 ) exp Mφ r τ) q φτ) ) ) dτ s. t 0 φτ) 4.12) By 4.7c) it follows that for every q 0there exists a finite time T := T q) 0, such that 1 φt) 2 Mφt) q φ r t) for all t T. This implies + 0 Mφ r τ) q φτ) ) φτ) dτ =+ for all q 0 and consequently by 4.12), we have that 0 Ris φ-rgas for the closedloop system 4.5) with x 2 = k 1 t, x 1 ) + d x 1, d [ 1, 1]. Byii) of Lemma 2.4 and definition 4.10c) it also follows that 0 Ris φ-rgas for the closed-loop system 4.5) with x 2 = k 1 t, x 1 ) + d x 1, d [ 1, 1]. Consider next the two-dimensional subsystem ẋ 1 = f 1 t,θ,x 1 ) + g 1 t,θ,x 1 )x 2 ẋ 2 = f 2 t,θ,x 1, x 2 ) + g 1 t,θ,x 1, x 2 )x 3 with x 3 as input. We apply Lemma 3.1 for this system. Clearly, by the previous analysis hypothesis H1) is satisfied for φ ) K as defined by 4.10c), γs) := s and µ = 0. Hypothesis H2) is trivially satisfied, while hypotheses H3) and H4) are consequences of inequalities 4.1), 4.2), 4.10a), 4.10b). The desired conclusion follows from the application of Lemma 3.1. The proof is complete. The following proposition is concerned with the problem of partial-state robust feedback stabilization of uncertain nonlinear time-varying systems. It is the analogue of Corollary 3.4 in [11] and Theorem 2.4 in [12], although here we consider uncertain systems. Its proof follows directly by induction and Lemmas 3.1 and 3.2. PROPOSITION 4.2 Consider the system 1.4), where z R m, x = x 1,...x n ) T R n, θ Ω R l, Ω is a compact set, f i i = 0,...,n) and g i i = 1,...,n) are measurable with respect to t 0, C 0 with respect to θ Ω and locally Lipschitz with respect to z, x), uniformly in θ Ω. Suppose that there exist functions φ K, a K con, constants δ 0 and K > 0, such that the following hold for all t, z, x,θ) R + R m R n Ω and i = 1,...,n: f 0 t,θ,z, x 1 ) aφt) z T, x 1 ) ) 4.13) f i t,θ,z, x 1,...,x i ) aφt) z T, x 1,...,x i ) ) 4.14) 1 K φ δ t) g it,θ,z, x 1,...,x i )) φt) + aφt) z T, x 1,...,x i ) ). 4.15) Suppose, furthermore, that 0 R m is φ-rgas for the following system ż = f 0 t,θ,z, d γ z ) ) φ µ 4.16) t)

16 434 I. KARAFYLLIS with θ, d) D := Ω [ 1, 1] as input, where µ 0 and γ K is a locally Lipschitz function that satisfies the following inequality for certain constants η, Λ > 0: Λs γs), s [0,η]. 4.17) Then for every locally Lipschitz function Γ ) K there exists a C mapping k : R + R n Rwith k, 0) = 0, such that 0 R m R n is φ-rgas for the following system: ż = f 0 t,θ,z, x 1 ) ẋ i = f i t,θ,z, x 1,...,x i ) + g i t,θ,z, x 1,...,x i )x i+1 i = 1,...,n 4.18) x n+1 = kt, x) + dγ z, x) ) with θ, d) D := Ω [ 1, 1] as input. Moreover, when φ ) is bounded then the mapping k can be chosen to be independent of t. EXAMPLE 4.3 Consider the system: ż = 2tz + θ 1 t) expµt)x ẋ = expat)θ 2 t)wz, x) + u 4.19) z, x) R 2, t 0, u R,θ = θ 1,θ 2 ) B0, r) where a, r, µ > 0 are known constants, wz, x) is a locally Lipschitz function satisfying w0, 0) = 0 and θ denotes the vector of the uncertain parameters of the system. It is immediate to verify that 0 Ris e t -RGAS for the subsystem ż = 2tz + θ 1 t)dt) z 4.20) where dt) 1. Indeed, for every θ ), d )) M B0,r) [ 1,1] the solution of 4.20) satisfies the estimate { )} zt) exp rt t 0 ) t 2 t0 2 z 0. Thus by Proposition 4.2 there exists a C mapping k :R + R Rwith k, 0) = 0 with such that the origin for 4.19) with u = kt, x) is e t -RGAS. 5. Applications to autonomous control systems In this section we study the applications of time-varying feedback laws to autonomous control systems. We first consider the case 1.5). We establish that the use of time-varying feedback can robustly accelerate the rate of convergence of the solution to the equilibrium point. This is shown by the following corollary, which is an immediate consequence of Proposition 4.1 and Lemma 2.7. COROLLARY 5.1 Consider system 1.5), where x = x 1,...x n ) T R n, θ Ω R l, Ω being a compact set, f i and g i are continuous with respect to θ Ω and locally Lipschitz with respect to x 1,...x i ), uniformly in θ Ω, with f i θ, 0,...,0) = 0, for all θ Ω,

17 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 435 for i = 1,...,n. Suppose that there exists a constant K > 0 such that the following hold for all x,θ) R n Ω and i = 1,...,n: 1 K g iθ, x 1,...,x i ). 5.1) Then for every φ ) K and Γ ) K being locally Lipschitz, there exists a C mapping k :R + R n Rwith k, 0) = 0, a function η ) K con and a constant p 0, with kt, x) η φ p t) x ), t, x) R + R n 5.2) such that 0 R n is φ-rgas for the following system with θ, d) D := Ω [ 1, 1] as input: ẋ i = f i θ, x 1,...,x i ) + g i θ, x 1,...,x i )x i+1 i = 1,...,n x n+1 = kt, x) + dγ x ). 5.3) Proof. Let φ ) K. Since each f i and g i is locally Lipschitz, uniformly in θ Ω, Lemma 2.7 implies that there exists a function a K con,such that the following inequalities hold for all t,θ,x) R + Ω R n and i = 1,...,n: f i θ, x 1,...,x i ) a x 1,...,x i ) ) aφt) x 1,...,x i ) ) 5.4a) g i θ, x 1,...,x i ) g i θ, 0,...,0) a x 1,...,x i ) ) aφt) x 1,...,x i ) ). 5.4b) Furthermore, inequality 5.1) gives for i = 1,...,n: 1 K φt) 1 K g iθ, x 1,...,x i ). 5.4c) Inequalities 5.4a) 5.4c) establish that all hypotheses of Proposition 4.1 are fulfilled for φt) = Rφt), where R := 1+sup θ Ω,i=1,...,n g i θ, 0,...,0). Notice that it holds: φt) φt) for all t 0. Therefore for every locally Lipschitz function Γ ) K, there exists a C mapping k : R + R n R,afunction η ) K con,aconstant p 0, with kt, x) ηφ p t) x ), such that 0 R n is φ-rgas for 3.63) with θ, d) Ω [ 1, 1] as input. Consequently, by Lemma 2.4 and inequality φt) φt), itfollows that 0 R n is φ-rgas for 5.3) with θ, d) Ω [ 1, 1] as input. Moreover, 5.2) is satisfied for ηs) := ηr p s). REMARK 5.2 Notice that the origin for system 1.5) cannot become φ-rgas for φt) = expt) with the application of locally Lipschitz static time-invariant feedback i.e. the rate of convergence to 0 R n of the solution of the closed-loop system 1.5) with a static locally Lipschitz time-invariant feedback cannot be faster than the exponential rate). EXAMPLE 5.3 Consider the two dimensional system ẋ 1 = θt)x x 2 ẋ 2 = u x 1, x 2 ) R 2, u R 5.5)

18 436 I. KARAFYLLIS where θ ) :R + [ 1, 1] is an unknown time-varying parameter. Let φ ) K be φt) a function that satisfies lim t + φ r t) = 0, for some constant r 1. Then 0 R 2 is φ-rgas for the following system with θ, d) [ 1, 1] 2 as input: ẋ 1 = θt)x x 2 ẋ 2 = kt, x 1, x 2 ) + dt) x 1 +dt) x 2 5.6) where kt, x 1, x 2 ) is the C time-varying feedback law, defined for some M > 0 sufficiently large, by the following relation: kt, x 1, x 2 ) := Mφ 2r t) z + z 3 + z 5) z := x 2 + 3φ r t) x 1 + x1 3 ) 5.7). Notice that for the selection φt) 1 K, the feedback law defined by 5.7) is actually time-invariant and guarantees uniform global asymptotic stability of the origin for system 5.6). Next we consider the problem of partial-state feedback stabilization of autonomous systems of the form 1.6). In the literature the usual assumption is that subsystem 1.6a) is ISS with x, u) as input. Here we intend to relax this hypothesis, by making use of time-varying feedback of the form u = kt, x). THEOREM 5.4 Consider the system 1.6) and suppose that there exists a constant K > 0, such that the following hold for all x,θ) R n Ω and i = 1,...,n: 1 K g iθ, x 1,...,x i ). 5.8) Furthermore suppose that the subsystem ż = f 0 z, x, u) is forward complete with x, u) as input and that 0 R m is GAS for the system ż = f 0 z, 0, 0). Then for every locally Lipschitz function Γ ) K there exists a C mapping k : R + R n R, with kt, 0) = 0, for all t 0, such that 0 R m R n is RGAS for the following system with θ, d) D := Ω [ 1, 1] as input: ż = f 0 z, x, u) ẋ i = f i θ, x 1,...,x i ) + g i θ, x 1,...,x i )x i+1 i = 1,...,n u = x n+1 = kt, x) + dγ x ). 5.9) Proof. The proof is divided into three parts. First part. We obtain estimates for the solution zt) of the subsystem 1.6a), with x, u) R n Ras input. Second part. We design a feedback law kt, x), such that 0 R n is φ-rgas for the subsystem 1.6b) with x n+1 = kt, x) + dγ x ), for an appropriate choice of φ K. Third part. We prove that 0 R m R n is RGAS for 5.9).

19 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 437 First part Since 0 R m is GAS for the subsystem ż = f 0 z, 0, 0), then in Angeli et al. 2000, Lemma IV.10) and Sontag 1998, Theorem 3), there exists a smooth function V :R n R +, K functions a 1, a 2,λ,δ, such that for all z, x, u) R m R n Rwe have a 1 z ) V z) a 2 z ) 5.10a) V z z) f 0z, x, u) V z) + λ z )δ x, u) ). 5.10b) Furthermore, in Angeli & Sontag 1999, Corollary 2.11), there exists a smooth and proper function W :R n R + and functions a 3, a 4,σ of class K and a constant R > 0, such that for all z, x, u) R m R n Rwe have a 3 z ) W z) a 4 z ) + R 5.10c) W z z) f 0z, x, u) W z) + σ x, u) ). 5.10d) Notice that by virtue of 5.10c), 5.10d) the solution zt) initiated at zt 0 ) = z 0 of the subsystem 1.6a) satisfies a 3 zt) ) expt t 0 )a 4 z 0 ) + R) + t t 0 expt τ)σ xτ), uτ)) )dτ, t t ) On the other hand, by 5.10a), 5.10b) and 5.11) we obtain the estimate for λs) := λ2a 1 3 2s)) and for all ξ [t 0, t]: a 1 zt) ) exp t ξ))a 2 zξ) ) t τ + λ expτ s)σ xs), us)) )ds + ξ t ξ t 0 ) δ xτ), uτ)) )dτ λexpτ t 0 )a 4 z 0 ) + R))δ xτ), uτ)) )dτ, t ξ. 5.12) Second part In Sontag 1998, Corollary 10), there exist functions q 1, q 2,µ K C 0, + )), such that σrs) q 1 r)q 1 s), r, s a) δrs) q 2 r)q 2 s), r, s b) λrs) µr)µs), r, s c) Without loss of generality, we may assume that q 1 1, q 1 2 K C 0, + )). Define φt) := exp t)) + 1 q 1 q 1 2 exp t) µexpt)) ). 5.14a)

20 438 I. KARAFYLLIS Notice that φ K +. Consequently, by Lemma 2.2, there exists φ K such that φt) φt), t b) Furthermore, by 5.8) and Corollary 5.1, we have that for every locally Lipschitz function Γ ) K there exists a C mapping k :R + R n R,afunction η Q, aconstant p 0, with kt, x) η φ p t) x ), t, x) R + R n 5.15) such that 0 R n is φ-rgas for the following system with θ, d) D := Ω [ 1, 1] as input: ẋ i = f i θ, x 1,...,x i ) + g i θ, x 1,...,x i )x i+1 i = 1,...,n x n+1 = kt, x) + dγ x ). 5.16) Third part Since is φ-rgas for 5.16) with input θ, d) M D,byLemma 2.4 it follows that there exist a KL function ζ and a K + function β, such that φ p+1 t) xt) ζ βt 0 ) x 0, t t 0 ), t t ) where p 0isthe constant involved in 5.15). Moreover, applying Lemma 2.7 for the even extension of Γ ) on R which is locally Lipschitz), we find that there exists a function Γ ) K con such that Γ s) Γ s), s ) Inequalities 5.15), 5.17), 5.18) and the fact that Γ, η K con,imply that the following estimate holds for all t t 0 : xt), ut)) xt) + ut) = xt) + kt, xt)) + dt)γ xt) ) xt) +η φ p t) xt) ) + Γ xt) ) 1 + dη φ p t) xt) ) + d Γ φ p t) xt) )) φ p t) xt) ds ds 1 φt) H βt 0) x 0 ) ζ βt 0 ) x 0, t t 0 ) 5.19) where Hs) := 1+ dη d Γ ds ζs, 0))+ ds ζs, 0)) is a continuous, positive and non-decreasing function. By 5.13a) and 5.19) it follows that τ τ ) 1 expτ s)σ xs), us)) )ds expτ)q 1 Z βt 0 ) x 0 )) q 1 ds, τ t 0 t 0 t 0 φs) ) where Zs) := Hs)ζs, 0), Z K.Onthe other hand 5.14) implies that q 1 1 φt) exp t), which in conjunction with the latter inequality gives τ expτ s)σ xs), us)) )ds expτ)q 1 Z βt 0 ) x 0 )), τ t ) t 0

21 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 439 The above inequality, combined with 5.12), 5.13b), 5.13c) and 5.19) gives for all ξ [t 0, t]: a 1 zt) ) exp t ξ))a 2 zξ) ) +q 2 Z βt 0 ) x 0 )) [µ q 1 Z βt 0 ) x 0 ))) + µ a 4 z 0 ) + R)] I t,ξ) 5.21a) t ) 1 I t,ξ):= µexpτ))q 2 dτ. ξ φτ) 5.21b) ) As previously, using 5.14) we may establish that µexpt))q 1 2 φt) exp t) and thus a 1 zt) ) exp t ξ))a 2 zξ) ) + + exp ξ)q 2 Z βt 0 ) x 0 )) [ µ q 1 Z βt 0 ) x 0 ))) µ a 4 z 0 ) + R) ] for all ξ [t 0, t] and t ξ. 5.22) The inequality above and 5.17) imply that 0 R m R n is RGAS for 5.9). In order to establish this fact, notice that, by virtue of 5.17) and 5.22), for all T 0 and r 0, it holds sup { zt), xt)) ; θ, d) M D, t t 0, z 0, x 0 ) r, t 0 [0, T ]} GβT )r) 5.23a) Gs) := ζs, 0) + a 1 1 a 2 s) + q 2 Zs)) [µ q 1 Zs))) + µ R + a 4 s))]) 5.23b) where G is a class K function. This establishes stability. In order to prove attractivity let ε > 0, r > 0 and T 0. There exists a τ := τε,t, r) T, such that exp ξ)q 2 ZβT )r))[µq 1 ZβT )r))) + µa 4 r) + R)] a 1 ε), for all ξ τ. It follows from 5.17), 5.22) and 5.23) that for all t τ it holds sup { zt), xt)) ; θ, d) M D, z 0, x 0 ) r, t 0 [0, T ]} ζβt )r, t T ) + a 1 1 exp t τ))a 2GβT )r)) + a 1 ε)). This proves that lim sup { zt), xt)) ; θ, d) M D, z 0, x 0 ) r, t 0 [0, T ]} ε. t + Since ε>0isarbitrary we have that lim sup{ zt), xt)) ; θ, d) M D, z 0, x 0 ) r, t + t 0 [0, T ]} = 0. The proof is complete. Acknowledgements The author thanks Professor John Tsinias for his comments and his suggestions. REFERENCES ANGELI, D.& SONTAG, E. D.1999) Forward completeness, unbounded observability and their Lyapunov characterizations. Systems and Control Letters, 38, ANGELI, D., SONTAG, E. D.& WANG, Y.2000) A characterization of integral input-to-state stability. IEEE Trans. Automat. Contr., 45,

22 440 I. KARAFYLLIS FILLIPOV, A. F.1988) Differential Equations with Discontinuous Right-Hand Sides. Dordrecht: Kluwer. JIANG, Z.P.,TEEL, A.&PRALY, L.1994) Small-gain theorem for ISS systems and applications. Mathematics of Control, Signals and Systems, 7, KARAFYLLIS, I.& TSINIAS, J.2001) Converse Lyapunov Theorems for Non-Uniform In Time Global Asymptotic Stability and Stabilization By Means of Time-Varying Feedback. Proceedings of NOLCOS. KARAFYLLIS, I.& TSINIAS, J.2002a) Global stabilization and asymptotic tracking for a class of nonlinear systems by means of time-varying feedback. Int. Journal of Robust and Nonlinear Control, toappear. KARAFYLLIS, I.& TSINIAS, J.2002b) A converse Lyapunov theorem for non-uniform in time global asymptotic stability and its application to feedback stabilization. SIAM Journal Control and Optimization, submitted. KHALIL, H.K.1996) Nonlinear Systems, 2nd Edition. Englewood Cliffs, NJ: Prentice-Hall. PANTELEY, E.& LORIA, A.1998) On global uniform asymptotic stability of nonlinear timevarying systems in cascade. Systems and Control Letters, 33, SONTAG, E. D.1998) Comments on integral variants of ISS. Systems and Control Letters, 34, TSINIAS, J.1996) Versions of Sontag s input to state stability condition and output feedback stabilization. J. Math. Systems Estimation and Control, 6, TSINIAS, J.2000) Backstepping design for time-varying nonlinear systems with unknown parameters. Systems and Control Letters, 39, TSINIAS, J.& KARAFYLLIS, I.1999) ISS property for time-varying systems and application to partial-static feedback stabilization and asymptotic tracking. IEEE Trans. Automat. Contr., 44, Appendix Proof of Lemma 2.2. The implications i) iii) are obvious. We only prove the last statement of the lemma. Define the function { φlog s) + s if s 1 µs) := A.1) φ0) + 1)s if 0 s < 1. Clearly µ ) K and satisfies Define the function φt) µ e t), t 0. A.2) { 0 if s = 0 ρs) := 1 ) µ 1 1s if 0 < s. A.3) Again we have that ρ ) K and let ρ ) K C 0, + )) be a function with d ρ ds s) 1 for all s > 0 and lim s 0 ρs) + s =+, that satisfies ρs) ρs) for all s 0. Thus by A.3) we have 1 ) ρs) s > 0 µ e t) 1 µ 1 1s ρ 1 e t) t 0. A.4)

23 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 441 Define φt) := 1 ρ 1 e t). A.5) Since ρ ) K C 0, + )) with d ρ ds s) 1 for all s > 0, we easily establish that φ ) C R + ) and that φ ) is non-decreasing. Furthermore, since d ρ ds s) 1 for all s > 0 and lim ρs) s 0 + s =+,itfollows that 0 d ρ 1 ds s) 1, for all s 0. This fact and definition A.5) imply d φ dt t) = φ 2 t) d ρ 1 e t ) e t φ 2 t)e t. ds 1 d φ The latter inequality gives lim t + φ 2 t) dt t) = 0. Notice that we can easily establish using the implied inequality ρ 1 s) s for all s 0) that φt) e t 1, for all t 0. Consequently, we conclude that φ ) K. Moreover, by A.2), A.4) and definition A.5) we get that φt) φt), for all t 0. The proof is complete. Proof of Lemma 2.4. Implications i) and ii) are immediate consequences of the definition of φ-rgas and the fact that φt) 1, for all t 0. We focus on implication iii). Let p 0 and consider the time-varying transformation z := φ p t)x. A.6) Clearly, zt) satisfies the following system of differential equations: ż = p φt) ) φt) z + φ p z t) f t, φ p t), d z R n, t 0, d D. The fact that 0 R n is φ-rgas for 1.1) and definition A.6) imply that 0 R n is RGAS for the system above with d as input. Furthermore, Proposition 2.2 in Karafyllis & Tsinias 2002b) guarantees the existence of a KL function σ ) and a K + function β ) such that ) zt) σ βt 0 ) z 0, t t 0, t t 0. A.7) The desired 2.2) is a consequence of inequality A.7), definition A.6) and the selection βt) := βt)φ p t). Proof of Lemma 2.6. The statements i) ii) are obvious. We prove statements iii) iv). iii) Define the function γs) := s + sup 0 τ s aτ). A.8) Clearly γ C 0 R + ) and is strictly increasing with as) γs), s 0. A.9)

24 442 I. KARAFYLLIS Let h : R R + be a C function with hs) = 0ifs / 0, 1) and R hs)ds = 1 0 hs)ds = 1. Define the function 1 γs) := γw)hw s)dw = γs + w)hw)dw. A.10) Clearly γ C R + ),isnon-decreasing and satisfies R 0 γs) γs) γs + 1), s 0. A.11) Let r > 0beanarbitrary constant and define the following functions: d γ δs) := ds r) + 1 if 0 s r sup r τ s d γ A.12) ds τ) + 1 if s > r βs) = s 0 δw)dw. A.13) Since by definition A.12), δ is continuous, non-decreasing and satisfies δs) 1, s 0, we have that β K con. Notice that for s > r we get by A.12) and A.13) βs) s r δw)dw γs) γr) and the latter inequality in conjunction with A.9) and A.11) implies that as) R+βs), s 0, for R = γr). iv) Inequality 2.3a) is a consequence of the inequality ȧs) ȧλs), which holds for all λ 1 and s 0. The right-hand side of inequality 2.3b) is a well-known property of the functions of class K. The left-hand side of inequality 2.3b) is a consequence of the inequality ȧs 1 ) ȧs 1 + s 2 ), which holds for all s 1 0 and s 2 0. The proof is complete. Proof of Lemma 2.7. Since f is locally Lipschitz in x, uniformly in θ, there exist constants L, r > 0, such that Consider the function f θ, x) L x, θ Ω, for x r. A.14) βs) := sup f θ, x). A.15) θ Ω x s Clearly, the mapping β ) is continuous and non-decreasing with β0) = 0. Furthermore by A.14) we have βs) Ls, for s r. A.16)

25 NON-UNIFORM STABILIZATION OF CONTROL SYSTEMS 443 2s Clearly the function ζs) = 1 s s βw)dw belongs to the class K C 1 0, + )) and satisfies ζs) βs) for all s 0. Define the functions: dζ r for 0 s < ds 2) r 2 δs) := dζ ds τ) for s r A.17) 2 sup r 2 τ s s as) := λs + δw)dw 0 A.18) { λ := max L + 1, 2 r r 2) } ζ. A.19) Since δ is a continuous, non-decreasing function we have that a K con.weclaim that 2.4) is satisfied. Notice that as) λs L + 1)s and consequently for all x r and θ Ω,weobtain using A.14) f θ, x) L x a x ). On the other hand, for s r 2,byA.17) and A.19) we have that r 2 s as) = λs + δw)dw + δw)dw λ r s r r 2 The proof is complete. dζ w)dw ζs) βs) ds Proof of Lemma 2.8. Let h :R + R + be a C function that satisfies hs) = 0, s / 0, 1) and R + hs)ds = 1 0 hs)ds = 1. Define ãs) := au)hu s)du au)hu)du. A.20) R + R + Notice that ã0) = 0 and ã C R + ). Furthermore, we have ãs) = 1 0 as + w) aw))hw)dw. A.21) Clearly by virtue of 2.3b) of Lemma 2.6 and A.21), it follows that 2.5) holds. Moreover by A.21) we get dã 1 ds s) = da s + w)hw)dw 0 ds A.22) which implies that dã ds s) is non-decreasing and positive. Therefore ã K con C R + ). Define R := da ds 2r) for some r > 0 and notice that we also have as) Rs, s [0, 2r]. A.23)

26 444 I. KARAFYLLIS Finally, define βs) := Rs Rs + exp for 0 s r 1 r 1 ) ãs) for s > r. s r A.24) Clearly β C R + ) and its odd extension β ) is also a smooth function on R. Moreover by 2.5), A.23) and definition A.24) we have that as) βs), s 0. By virtue of iii) of Lemma 2.6, there exist M > 0 and δ K con such that dã ds s) M + δs) and since ) 1 sup s>0 exp 1 s 2 s 4, we can easily verify that 2.6) and 2.7) are satisfied for ) 1 R := R + M exp r γs) := 5exp ) 1 ãs) + δs)) + Rs. r The proof is complete. Proof of Lemma 2.9. In order to prove 2.10), let r 0, t 0 0, t t 0 and notice that for the solution βt, t 0, r) of 2.11) we have τ βt τ,t 0, r) = ρφt τ)βt τ,t 0, r)), τ [0, t t 0 ]. A.25) Let a vector x B βt,t0,r) be the initial condition for the problem dξ τ) = f t τ,ξ,d) dτ ξ0) = x, d D,τ 0. A.26) This is the time-reversed system 1.1). It is clear by virtue of 2.8) that the following differential inequality is satisfied: D + ξτ) ρφt τ) ξτ) ), τ [0, t]. A.27) It follows by A.25), A.27) and the comparison Lemma in Khalil 1996), that ξτ) βt τ,t 0, r), τ [0, t t 0 ]. A.28) Since βt 0, t 0, r) = r, inequality A.28) shows that there exists x 0 B r and d M D such that xt, t 0, x 0 ; d) = x and it is given by x 0 = ξt t 0 ) for the particular d M D. Since x B βt,t0,r) is arbitrary, it follows that 2.10) holds. The proof is complete.

Nonuniform in time state estimation of dynamic systems

Nonuniform in time state estimation of dynamic systems Systems & Control Letters 57 28 714 725 www.elsevier.com/locate/sysconle Nonuniform in time state estimation of dynamic systems Iasson Karafyllis a,, Costas Kravaris b a Department of Environmental Engineering,

More information

Converse Lyapunov theorem and Input-to-State Stability

Converse Lyapunov theorem and Input-to-State Stability Converse Lyapunov theorem and Input-to-State Stability April 6, 2014 1 Converse Lyapunov theorem In the previous lecture, we have discussed few examples of nonlinear control systems and stability concepts

More information

Observer design for a general class of triangular systems

Observer design for a general class of triangular systems 1st International Symposium on Mathematical Theory of Networks and Systems July 7-11, 014. Observer design for a general class of triangular systems Dimitris Boskos 1 John Tsinias Abstract The paper deals

More information

Can we prove stability by using a positive definite function with non sign-definite derivative?

Can we prove stability by using a positive definite function with non sign-definite derivative? IMA Journal of Mathematical Control and Information (2012), 147 170 doi:10.1093/imamci/dnr035 Advance Access publication on November 28, 2011 Can we prove stability by using a positive definite function

More information

Numerical schemes for nonlinear predictor feedback

Numerical schemes for nonlinear predictor feedback Math. Control Signals Syst. 204 26:59 546 DOI 0.007/s00498-04-027-9 ORIGINAL ARTICLE Numerical schemes for nonlinear predictor feedback Iasson Karafyllis Miroslav Krstic Received: 3 October 202 / Accepted:

More information

Robust output feedback stabilization and nonlinear observer design

Robust output feedback stabilization and nonlinear observer design Systems & Control Letters 54 (2005) 925 938 www.elsevier.com/locate/sysconle Robust output feedback stabilization and nonlinear observer design Iasson Karafyllis a,, Costas Kravaris b a Division of Mathematics,

More information

An asymptotic ratio characterization of input-to-state stability

An asymptotic ratio characterization of input-to-state stability 1 An asymptotic ratio characterization of input-to-state stability Daniel Liberzon and Hyungbo Shim Abstract For continuous-time nonlinear systems with inputs, we introduce the notion of an asymptotic

More information

L -Bounded Robust Control of Nonlinear Cascade Systems

L -Bounded Robust Control of Nonlinear Cascade Systems L -Bounded Robust Control of Nonlinear Cascade Systems Shoudong Huang M.R. James Z.P. Jiang August 19, 2004 Accepted by Systems & Control Letters Abstract In this paper, we consider the L -bounded robust

More information

On Sontag s Formula for the Input-to-State Practical Stabilization of Retarded Control-Affine Systems

On Sontag s Formula for the Input-to-State Practical Stabilization of Retarded Control-Affine Systems On Sontag s Formula for the Input-to-State Practical Stabilization of Retarded Control-Affine Systems arxiv:1206.4240v1 [math.oc] 19 Jun 2012 P. Pepe Abstract In this paper input-to-state practically stabilizing

More information

1 The Observability Canonical Form

1 The Observability Canonical Form NONLINEAR OBSERVERS AND SEPARATION PRINCIPLE 1 The Observability Canonical Form In this Chapter we discuss the design of observers for nonlinear systems modelled by equations of the form ẋ = f(x, u) (1)

More information

An homotopy method for exact tracking of nonlinear nonminimum phase systems: the example of the spherical inverted pendulum

An homotopy method for exact tracking of nonlinear nonminimum phase systems: the example of the spherical inverted pendulum 9 American Control Conference Hyatt Regency Riverfront, St. Louis, MO, USA June -, 9 FrA.5 An homotopy method for exact tracking of nonlinear nonminimum phase systems: the example of the spherical inverted

More information

Feedback stabilization methods for the numerical solution of ordinary differential equations

Feedback stabilization methods for the numerical solution of ordinary differential equations Feedback stabilization methods for the numerical solution of ordinary differential equations Iasson Karafyllis Department of Environmental Engineering Technical University of Crete 731 Chania, Greece ikarafyl@enveng.tuc.gr

More information

On integral-input-to-state stabilization

On integral-input-to-state stabilization On integral-input-to-state stabilization Daniel Liberzon Dept. of Electrical Eng. Yale University New Haven, CT 652 liberzon@@sysc.eng.yale.edu Yuan Wang Dept. of Mathematics Florida Atlantic University

More information

IN [1], an Approximate Dynamic Inversion (ADI) control

IN [1], an Approximate Dynamic Inversion (ADI) control 1 On Approximate Dynamic Inversion Justin Teo and Jonathan P How Technical Report ACL09 01 Aerospace Controls Laboratory Department of Aeronautics and Astronautics Massachusetts Institute of Technology

More information

From convergent dynamics to incremental stability

From convergent dynamics to incremental stability 51st IEEE Conference on Decision Control December 10-13, 01. Maui, Hawaii, USA From convergent dynamics to incremental stability Björn S. Rüffer 1, Nathan van de Wouw, Markus Mueller 3 Abstract This paper

More information

Introduction to Nonlinear Control Lecture # 3 Time-Varying and Perturbed Systems

Introduction to Nonlinear Control Lecture # 3 Time-Varying and Perturbed Systems p. 1/5 Introduction to Nonlinear Control Lecture # 3 Time-Varying and Perturbed Systems p. 2/5 Time-varying Systems ẋ = f(t, x) f(t, x) is piecewise continuous in t and locally Lipschitz in x for all t

More information

Input to state Stability

Input to state Stability Input to state Stability Mini course, Universität Stuttgart, November 2004 Lars Grüne, Mathematisches Institut, Universität Bayreuth Part III: Lyapunov functions and quantitative aspects ISS Consider with

More information

c 2007 Society for Industrial and Applied Mathematics

c 2007 Society for Industrial and Applied Mathematics SIAM J. CONTROL OPTIM. Vol. 46, No. 4, pp. 1483 1517 c 2007 Society for Industrial and Applied Mathematics A SMALL-GAIN THEOREM FOR A WIDE CLASS OF FEEDBACK SYSTEMS WITH CONTROL APPLICATIONS IASSON KARAFYLLIS

More information

Global output regulation through singularities

Global output regulation through singularities Global output regulation through singularities Yuh Yamashita Nara Institute of Science and Techbology Graduate School of Information Science Takayama 8916-5, Ikoma, Nara 63-11, JAPAN yamas@isaist-naraacjp

More information

Converse Lyapunov-Krasovskii Theorems for Systems Described by Neutral Functional Differential Equation in Hale s Form

Converse Lyapunov-Krasovskii Theorems for Systems Described by Neutral Functional Differential Equation in Hale s Form Converse Lyapunov-Krasovskii Theorems for Systems Described by Neutral Functional Differential Equation in Hale s Form arxiv:1206.3504v1 [math.ds] 15 Jun 2012 P. Pepe I. Karafyllis Abstract In this paper

More information

An introduction to Mathematical Theory of Control

An introduction to Mathematical Theory of Control An introduction to Mathematical Theory of Control Vasile Staicu University of Aveiro UNICA, May 2018 Vasile Staicu (University of Aveiro) An introduction to Mathematical Theory of Control UNICA, May 2018

More information

The Rationale for Second Level Adaptation

The Rationale for Second Level Adaptation The Rationale for Second Level Adaptation Kumpati S. Narendra, Yu Wang and Wei Chen Center for Systems Science, Yale University arxiv:1510.04989v1 [cs.sy] 16 Oct 2015 Abstract Recently, a new approach

More information

Small Gain Theorems on Input-to-Output Stability

Small Gain Theorems on Input-to-Output Stability Small Gain Theorems on Input-to-Output Stability Zhong-Ping Jiang Yuan Wang. Dept. of Electrical & Computer Engineering Polytechnic University Brooklyn, NY 11201, U.S.A. zjiang@control.poly.edu Dept. of

More information

On robustness of suboptimal min-max model predictive control *

On robustness of suboptimal min-max model predictive control * Manuscript received June 5, 007; revised Sep., 007 On robustness of suboptimal min-max model predictive control * DE-FENG HE, HAI-BO JI, TAO ZHENG Department of Automation University of Science and Technology

More information

Lecture 4. Chapter 4: Lyapunov Stability. Eugenio Schuster. Mechanical Engineering and Mechanics Lehigh University.

Lecture 4. Chapter 4: Lyapunov Stability. Eugenio Schuster. Mechanical Engineering and Mechanics Lehigh University. Lecture 4 Chapter 4: Lyapunov Stability Eugenio Schuster schuster@lehigh.edu Mechanical Engineering and Mechanics Lehigh University Lecture 4 p. 1/86 Autonomous Systems Consider the autonomous system ẋ

More information

Further Equivalences and Semiglobal Versions of Integral Input to State Stability

Further Equivalences and Semiglobal Versions of Integral Input to State Stability Further Equivalences and Semiglobal Versions of Integral Input to State Stability David Angeli Dip. Sistemi e Informatica University of Florence 5139 Firenze, Italy angeli@dsi.unifi.it E. D. Sontag Department

More information

Nonlinear Systems and Control Lecture # 12 Converse Lyapunov Functions & Time Varying Systems. p. 1/1

Nonlinear Systems and Control Lecture # 12 Converse Lyapunov Functions & Time Varying Systems. p. 1/1 Nonlinear Systems and Control Lecture # 12 Converse Lyapunov Functions & Time Varying Systems p. 1/1 p. 2/1 Converse Lyapunov Theorem Exponential Stability Let x = 0 be an exponentially stable equilibrium

More information

On finite gain L p stability of nonlinear sampled-data systems

On finite gain L p stability of nonlinear sampled-data systems Submitted for publication in Systems and Control Letters, November 6, 21 On finite gain L p stability of nonlinear sampled-data systems Luca Zaccarian Dipartimento di Informatica, Sistemi e Produzione

More information

arxiv: v3 [math.ds] 22 Feb 2012

arxiv: v3 [math.ds] 22 Feb 2012 Stability of interconnected impulsive systems with and without time-delays using Lyapunov methods arxiv:1011.2865v3 [math.ds] 22 Feb 2012 Sergey Dashkovskiy a, Michael Kosmykov b, Andrii Mironchenko b,

More information

Decentralized Disturbance Attenuation for Large-Scale Nonlinear Systems with Delayed State Interconnections

Decentralized Disturbance Attenuation for Large-Scale Nonlinear Systems with Delayed State Interconnections Decentralized Disturbance Attenuation for Large-Scale Nonlinear Systems with Delayed State Interconnections Yi Guo Abstract The problem of decentralized disturbance attenuation is considered for a new

More information

A Novel Integral-Based Event Triggering Control for Linear Time-Invariant Systems

A Novel Integral-Based Event Triggering Control for Linear Time-Invariant Systems 53rd IEEE Conference on Decision and Control December 15-17, 2014. Los Angeles, California, USA A Novel Integral-Based Event Triggering Control for Linear Time-Invariant Systems Seyed Hossein Mousavi 1,

More information

A non-coercive Lyapunov framework for stability of distributed parameter systems

A non-coercive Lyapunov framework for stability of distributed parameter systems 17 IEEE 56th Annual Conference on Decision and Control (CDC December 1-15, 17, Melbourne, Australia A non-coercive Lyapunov framework for stability of distributed parameter systems Andrii Mironchenko and

More information

A LaSalle version of Matrosov theorem

A LaSalle version of Matrosov theorem 5th IEEE Conference on Decision Control European Control Conference (CDC-ECC) Orlo, FL, USA, December -5, A LaSalle version of Matrosov theorem Alessro Astolfi Laurent Praly Abstract A weak version of

More information

Backstepping Design for Time-Delay Nonlinear Systems

Backstepping Design for Time-Delay Nonlinear Systems Backstepping Design for Time-Delay Nonlinear Systems Frédéric Mazenc, Projet MERE INRIA-INRA, UMR Analyse des Systèmes et Biométrie, INRA, pl. Viala, 346 Montpellier, France, e-mail: mazenc@helios.ensam.inra.fr

More information

Disturbance Attenuation for a Class of Nonlinear Systems by Output Feedback

Disturbance Attenuation for a Class of Nonlinear Systems by Output Feedback Disturbance Attenuation for a Class of Nonlinear Systems by Output Feedback Wei in Chunjiang Qian and Xianqing Huang Submitted to Systems & Control etters /5/ Abstract This paper studies the problem of

More information

State-norm estimators for switched nonlinear systems under average dwell-time

State-norm estimators for switched nonlinear systems under average dwell-time 49th IEEE Conference on Decision and Control December 15-17, 2010 Hilton Atlanta Hotel, Atlanta, GA, USA State-norm estimators for switched nonlinear systems under average dwell-time Matthias A. Müller

More information

Stabilization in spite of matched unmodelled dynamics and An equivalent definition of input-to-state stability

Stabilization in spite of matched unmodelled dynamics and An equivalent definition of input-to-state stability Stabilization in spite of matched unmodelled dynamics and An equivalent definition of input-to-state stability Laurent Praly Centre Automatique et Systèmes École des Mines de Paris 35 rue St Honoré 7735

More information

1 Lyapunov theory of stability

1 Lyapunov theory of stability M.Kawski, APM 581 Diff Equns Intro to Lyapunov theory. November 15, 29 1 1 Lyapunov theory of stability Introduction. Lyapunov s second (or direct) method provides tools for studying (asymptotic) stability

More information

EN Nonlinear Control and Planning in Robotics Lecture 10: Lyapunov Redesign and Robust Backstepping April 6, 2015

EN Nonlinear Control and Planning in Robotics Lecture 10: Lyapunov Redesign and Robust Backstepping April 6, 2015 EN530.678 Nonlinear Control and Planning in Robotics Lecture 10: Lyapunov Redesign and Robust Backstepping April 6, 2015 Prof: Marin Kobilarov 1 Uncertainty and Lyapunov Redesign Consider the system [1]

More information

Uniform weak attractivity and criteria for practical global asymptotic stability

Uniform weak attractivity and criteria for practical global asymptotic stability Uniform weak attractivity and criteria for practical global asymptotic stability Andrii Mironchenko a a Faculty of Computer Science and Mathematics, University of Passau, Innstraße 33, 94032 Passau, Germany

More information

SYNCHRONIZATION OF NONAUTONOMOUS DYNAMICAL SYSTEMS

SYNCHRONIZATION OF NONAUTONOMOUS DYNAMICAL SYSTEMS Electronic Journal of Differential Equations, Vol. 003003, No. 39, pp. 1 10. ISSN: 107-6691. URL: http://ejde.math.swt.edu or http://ejde.math.unt.edu ftp ejde.math.swt.edu login: ftp SYNCHRONIZATION OF

More information

STABILITY ANALYSIS FOR NONLINEAR SYSTEMS WITH TIME-DELAYS. Shanaz Tiwari. A Dissertation Submitted to the Faculty of

STABILITY ANALYSIS FOR NONLINEAR SYSTEMS WITH TIME-DELAYS. Shanaz Tiwari. A Dissertation Submitted to the Faculty of STABILITY ANALYSIS FOR NONLINEAR SYSTEMS WITH TIME-DELAYS by Shanaz Tiwari A Dissertation Submitted to the Faculty of The Charles E. Schmidt College of Science in Partial Fulfillment of the Requirements

More information

A Systematic Approach to Extremum Seeking Based on Parameter Estimation

A Systematic Approach to Extremum Seeking Based on Parameter Estimation 49th IEEE Conference on Decision and Control December 15-17, 21 Hilton Atlanta Hotel, Atlanta, GA, USA A Systematic Approach to Extremum Seeking Based on Parameter Estimation Dragan Nešić, Alireza Mohammadi

More information

Stability Criteria for Interconnected iiss Systems and ISS Systems Using Scaling of Supply Rates

Stability Criteria for Interconnected iiss Systems and ISS Systems Using Scaling of Supply Rates Stability Criteria for Interconnected iiss Systems and ISS Systems Using Scaling of Supply Rates Hiroshi Ito Abstract This paper deals with problems of stability analysis of feedback and cascade interconnection

More information

Lyapunov Stability Theory

Lyapunov Stability Theory Lyapunov Stability Theory Peter Al Hokayem and Eduardo Gallestey March 16, 2015 1 Introduction In this lecture we consider the stability of equilibrium points of autonomous nonlinear systems, both in continuous

More information

Semi-global Robust Output Regulation for a Class of Nonlinear Systems Using Output Feedback

Semi-global Robust Output Regulation for a Class of Nonlinear Systems Using Output Feedback 2005 American Control Conference June 8-10, 2005. Portland, OR, USA FrC17.5 Semi-global Robust Output Regulation for a Class of Nonlinear Systems Using Output Feedback Weiyao Lan, Zhiyong Chen and Jie

More information

On Characterizations of Input-to-State Stability with Respect to Compact Sets

On Characterizations of Input-to-State Stability with Respect to Compact Sets On Characterizations of Input-to-State Stability with Respect to Compact Sets Eduardo D. Sontag and Yuan Wang Department of Mathematics, Rutgers University, New Brunswick, NJ 08903, USA Department of Mathematics,

More information

TTK4150 Nonlinear Control Systems Solution 6 Part 2

TTK4150 Nonlinear Control Systems Solution 6 Part 2 TTK4150 Nonlinear Control Systems Solution 6 Part 2 Department of Engineering Cybernetics Norwegian University of Science and Technology Fall 2003 Solution 1 Thesystemisgivenby φ = R (φ) ω and J 1 ω 1

More information

Observer-based quantized output feedback control of nonlinear systems

Observer-based quantized output feedback control of nonlinear systems Proceedings of the 17th World Congress The International Federation of Automatic Control Observer-based quantized output feedback control of nonlinear systems Daniel Liberzon Coordinated Science Laboratory,

More information

Convergence Rate of Nonlinear Switched Systems

Convergence Rate of Nonlinear Switched Systems Convergence Rate of Nonlinear Switched Systems Philippe JOUAN and Saïd NACIRI arxiv:1511.01737v1 [math.oc] 5 Nov 2015 January 23, 2018 Abstract This paper is concerned with the convergence rate of the

More information

LMI Methods in Optimal and Robust Control

LMI Methods in Optimal and Robust Control LMI Methods in Optimal and Robust Control Matthew M. Peet Arizona State University Lecture 15: Nonlinear Systems and Lyapunov Functions Overview Our next goal is to extend LMI s and optimization to nonlinear

More information

Nonlinear Control Systems

Nonlinear Control Systems Nonlinear Control Systems António Pedro Aguiar pedro@isr.ist.utl.pt 3. Fundamental properties IST-DEEC PhD Course http://users.isr.ist.utl.pt/%7epedro/ncs2012/ 2012 1 Example Consider the system ẋ = f

More information

A small-gain type stability criterion for large scale networks of ISS systems

A small-gain type stability criterion for large scale networks of ISS systems A small-gain type stability criterion for large scale networks of ISS systems Sergey Dashkovskiy Björn Sebastian Rüffer Fabian R. Wirth Abstract We provide a generalized version of the nonlinear small-gain

More information

Finite-time stability and input-to-state stability of stochastic nonlinear systems

Finite-time stability and input-to-state stability of stochastic nonlinear systems Finite-time stability and input-to-state stability of stochastic nonlinear systems KANG Yu, ZHAO Ping,. Department of Automation, University of Science and Technology of China, Hefei 36, Anhui, P. R. China

More information

Nonlinear Systems and Control Lecture # 19 Perturbed Systems & Input-to-State Stability

Nonlinear Systems and Control Lecture # 19 Perturbed Systems & Input-to-State Stability p. 1/1 Nonlinear Systems and Control Lecture # 19 Perturbed Systems & Input-to-State Stability p. 2/1 Perturbed Systems: Nonvanishing Perturbation Nominal System: Perturbed System: ẋ = f(x), f(0) = 0 ẋ

More information

Anti-synchronization of a new hyperchaotic system via small-gain theorem

Anti-synchronization of a new hyperchaotic system via small-gain theorem Anti-synchronization of a new hyperchaotic system via small-gain theorem Xiao Jian( ) College of Mathematics and Statistics, Chongqing University, Chongqing 400044, China (Received 8 February 2010; revised

More information

Passivity-based Stabilization of Non-Compact Sets

Passivity-based Stabilization of Non-Compact Sets Passivity-based Stabilization of Non-Compact Sets Mohamed I. El-Hawwary and Manfredi Maggiore Abstract We investigate the stabilization of closed sets for passive nonlinear systems which are contained

More information

On the construction of ISS Lyapunov functions for networks of ISS systems

On the construction of ISS Lyapunov functions for networks of ISS systems Proceedings of the 17th International Symposium on Mathematical Theory of Networks and Systems, Kyoto, Japan, July 24-28, 2006 MoA09.1 On the construction of ISS Lyapunov functions for networks of ISS

More information

Exponential stability of families of linear delay systems

Exponential stability of families of linear delay systems Exponential stability of families of linear delay systems F. Wirth Zentrum für Technomathematik Universität Bremen 28334 Bremen, Germany fabian@math.uni-bremen.de Keywords: Abstract Stability, delay systems,

More information

c 2002 Society for Industrial and Applied Mathematics

c 2002 Society for Industrial and Applied Mathematics SIAM J. CONTROL OPTIM. Vol. 4, No. 6, pp. 888 94 c 22 Society for Industrial and Applied Mathematics A UNIFYING INTEGRAL ISS FRAMEWORK FOR STABILITY OF NONLINEAR CASCADES MURAT ARCAK, DAVID ANGELI, AND

More information

Input to state Stability

Input to state Stability Input to state Stability Mini course, Universität Stuttgart, November 2004 Lars Grüne, Mathematisches Institut, Universität Bayreuth Part IV: Applications ISS Consider with solutions ϕ(t, x, w) ẋ(t) =

More information

Robust Stabilization of Non-Minimum Phase Nonlinear Systems Using Extended High Gain Observers

Robust Stabilization of Non-Minimum Phase Nonlinear Systems Using Extended High Gain Observers 28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June 11-13, 28 WeC15.1 Robust Stabilization of Non-Minimum Phase Nonlinear Systems Using Extended High Gain Observers Shahid

More information

Chapter III. Stability of Linear Systems

Chapter III. Stability of Linear Systems 1 Chapter III Stability of Linear Systems 1. Stability and state transition matrix 2. Time-varying (non-autonomous) systems 3. Time-invariant systems 1 STABILITY AND STATE TRANSITION MATRIX 2 In this chapter,

More information

L 2 -induced Gains of Switched Systems and Classes of Switching Signals

L 2 -induced Gains of Switched Systems and Classes of Switching Signals L 2 -induced Gains of Switched Systems and Classes of Switching Signals Kenji Hirata and João P. Hespanha Abstract This paper addresses the L 2-induced gain analysis for switched linear systems. We exploit

More information

Quasi-ISS Reduced-Order Observers and Quantized Output Feedback

Quasi-ISS Reduced-Order Observers and Quantized Output Feedback Joint 48th IEEE Conference on Decision and Control and 28th Chinese Control Conference Shanghai, P.R. China, December 16-18, 2009 FrA11.5 Quasi-ISS Reduced-Order Observers and Quantized Output Feedback

More information

Convergent systems: analysis and synthesis

Convergent systems: analysis and synthesis Convergent systems: analysis and synthesis Alexey Pavlov, Nathan van de Wouw, and Henk Nijmeijer Eindhoven University of Technology, Department of Mechanical Engineering, P.O.Box. 513, 5600 MB, Eindhoven,

More information

A SIMPLE EXTENSION OF CONTRACTION THEORY TO STUDY INCREMENTAL STABILITY PROPERTIES

A SIMPLE EXTENSION OF CONTRACTION THEORY TO STUDY INCREMENTAL STABILITY PROPERTIES A SIMPLE EXTENSION OF CONTRACTION THEORY TO STUDY INCREMENTAL STABILITY PROPERTIES Jérôme Jouffroy IFREMER - Underwater Robotics, Navigation Vision Department (RNV) Centre de Toulon Zone portuaire du Brégaillon

More information

Global Stability and Asymptotic Gain Imply Input-to-State Stability for State-Dependent Switched Systems

Global Stability and Asymptotic Gain Imply Input-to-State Stability for State-Dependent Switched Systems 2018 IEEE Conference on Decision and Control (CDC) Miami Beach, FL, USA, Dec. 17-19, 2018 Global Stability and Asymptotic Gain Imply Input-to-State Stability for State-Dependent Switched Systems Shenyu

More information

High-Gain Observers in Nonlinear Feedback Control. Lecture # 3 Regulation

High-Gain Observers in Nonlinear Feedback Control. Lecture # 3 Regulation High-Gain Observers in Nonlinear Feedback Control Lecture # 3 Regulation High-Gain ObserversinNonlinear Feedback ControlLecture # 3Regulation p. 1/5 Internal Model Principle d r Servo- Stabilizing u y

More information

L 1 Adaptive Controller for a Class of Systems with Unknown

L 1 Adaptive Controller for a Class of Systems with Unknown 28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June -3, 28 FrA4.2 L Adaptive Controller for a Class of Systems with Unknown Nonlinearities: Part I Chengyu Cao and Naira Hovakimyan

More information

High-Gain Observers in Nonlinear Feedback Control

High-Gain Observers in Nonlinear Feedback Control High-Gain Observers in Nonlinear Feedback Control Lecture # 1 Introduction & Stabilization High-Gain ObserversinNonlinear Feedback ControlLecture # 1Introduction & Stabilization p. 1/4 Brief History Linear

More information

Comments on integral variants of ISS 1

Comments on integral variants of ISS 1 Systems & Control Letters 34 (1998) 93 1 Comments on integral variants of ISS 1 Eduardo D. Sontag Department of Mathematics, Rutgers University, Piscataway, NJ 8854-819, USA Received 2 June 1997; received

More information

Explicit computation of the sampling period in emulation of controllers for nonlinear sampled-data systems

Explicit computation of the sampling period in emulation of controllers for nonlinear sampled-data systems Explicit computation of the sampling period in emulation of controllers for nonlinear sampled-data systems D. Nešić, A.R. Teel and D. Carnevale Abstract The purpose of this note is to apply recent results

More information

ADAPTIVE FEEDBACK LINEARIZING CONTROL OF CHUA S CIRCUIT

ADAPTIVE FEEDBACK LINEARIZING CONTROL OF CHUA S CIRCUIT International Journal of Bifurcation and Chaos, Vol. 12, No. 7 (2002) 1599 1604 c World Scientific Publishing Company ADAPTIVE FEEDBACK LINEARIZING CONTROL OF CHUA S CIRCUIT KEVIN BARONE and SAHJENDRA

More information

Local ISS of large-scale interconnections and estimates for stability regions

Local ISS of large-scale interconnections and estimates for stability regions Local ISS of large-scale interconnections and estimates for stability regions Sergey N. Dashkovskiy,1,a,2, Björn S. Rüffer 1,b a Zentrum für Technomathematik, Universität Bremen, Postfach 330440, 28334

More information

Global Stability and Asymptotic Gain Imply Input-to-State Stability for State-Dependent Switched Systems

Global Stability and Asymptotic Gain Imply Input-to-State Stability for State-Dependent Switched Systems Global Stability and Asymptotic Gain Imply Input-to-State Stability for State-Dependent Switched Systems Shenyu Liu Daniel Liberzon Abstract In this paper we study several stability properties for state-dependent

More information

A framework for stabilization of nonlinear sampled-data systems based on their approximate discrete-time models

A framework for stabilization of nonlinear sampled-data systems based on their approximate discrete-time models 1 A framework for stabilization of nonlinear sampled-data systems based on their approximate discrete-time models D.Nešić and A.R.Teel Abstract A unified framework for design of stabilizing controllers

More information

A NONLINEAR TRANSFORMATION APPROACH TO GLOBAL ADAPTIVE OUTPUT FEEDBACK CONTROL OF 3RD-ORDER UNCERTAIN NONLINEAR SYSTEMS

A NONLINEAR TRANSFORMATION APPROACH TO GLOBAL ADAPTIVE OUTPUT FEEDBACK CONTROL OF 3RD-ORDER UNCERTAIN NONLINEAR SYSTEMS Copyright 00 IFAC 15th Triennial World Congress, Barcelona, Spain A NONLINEAR TRANSFORMATION APPROACH TO GLOBAL ADAPTIVE OUTPUT FEEDBACK CONTROL OF RD-ORDER UNCERTAIN NONLINEAR SYSTEMS Choon-Ki Ahn, Beom-Soo

More information

Gramians based model reduction for hybrid switched systems

Gramians based model reduction for hybrid switched systems Gramians based model reduction for hybrid switched systems Y. Chahlaoui Younes.Chahlaoui@manchester.ac.uk Centre for Interdisciplinary Computational and Dynamical Analysis (CICADA) School of Mathematics

More information

Input-to-state stability of time-delay systems: criteria and open problems

Input-to-state stability of time-delay systems: criteria and open problems 217 IEEE 56th Annual Conference on Decision and Control (CDC) December 12-15, 217, Melbourne, Australia Input-to-state stability of time-delay systems: criteria and open problems Andrii Mironchenko and

More information

Monotone Control System. Brad C. Yu SEACS, National ICT Australia And RSISE, The Australian National University June, 2005

Monotone Control System. Brad C. Yu SEACS, National ICT Australia And RSISE, The Australian National University June, 2005 Brad C. Yu SEACS, National ICT Australia And RSISE, The Australian National University June, 005 Foreword The aim of this presentation is to give a (primitive) overview of monotone systems and monotone

More information

HIGHER ORDER SLIDING MODES AND ARBITRARY-ORDER EXACT ROBUST DIFFERENTIATION

HIGHER ORDER SLIDING MODES AND ARBITRARY-ORDER EXACT ROBUST DIFFERENTIATION HIGHER ORDER SLIDING MODES AND ARBITRARY-ORDER EXACT ROBUST DIFFERENTIATION A. Levant Institute for Industrial Mathematics, 4/24 Yehuda Ha-Nachtom St., Beer-Sheva 843, Israel Fax: +972-7-232 and E-mail:

More information

Output Feedback Stabilization with Prescribed Performance for Uncertain Nonlinear Systems in Canonical Form

Output Feedback Stabilization with Prescribed Performance for Uncertain Nonlinear Systems in Canonical Form Output Feedback Stabilization with Prescribed Performance for Uncertain Nonlinear Systems in Canonical Form Charalampos P. Bechlioulis, Achilles Theodorakopoulos 2 and George A. Rovithakis 2 Abstract The

More information

A Generalization of Barbalat s Lemma with Applications to Robust Model Predictive Control

A Generalization of Barbalat s Lemma with Applications to Robust Model Predictive Control A Generalization of Barbalat s Lemma with Applications to Robust Model Predictive Control Fernando A. C. C. Fontes 1 and Lalo Magni 2 1 Officina Mathematica, Departamento de Matemática para a Ciência e

More information

Navigation and Obstacle Avoidance via Backstepping for Mechanical Systems with Drift in the Closed Loop

Navigation and Obstacle Avoidance via Backstepping for Mechanical Systems with Drift in the Closed Loop Navigation and Obstacle Avoidance via Backstepping for Mechanical Systems with Drift in the Closed Loop Jan Maximilian Montenbruck, Mathias Bürger, Frank Allgöwer Abstract We study backstepping controllers

More information

L 1 Adaptive Controller for Multi Input Multi Output Systems in the Presence of Unmatched Disturbances

L 1 Adaptive Controller for Multi Input Multi Output Systems in the Presence of Unmatched Disturbances 28 American Control Conference Westin Seattle Hotel, Seattle, Washington, USA June -3, 28 FrA4.4 L Adaptive Controller for Multi Input Multi Output Systems in the Presence of Unmatched Disturbances Chengyu

More information

Further Results on Input-to-State Stability for Nonlinear Systems with Delayed Feedbacks

Further Results on Input-to-State Stability for Nonlinear Systems with Delayed Feedbacks Further Results on Input-to-State Stability for Nonlinear Systems with Delayed Feedbacks Frédéric Mazenc a, Michael Malisoff b,, Zongli Lin c a Projet MERE INRIA-INRA, UMR Analyse des Systèmes et Biométrie

More information

Nonlinear Tracking Control of Underactuated Surface Vessel

Nonlinear Tracking Control of Underactuated Surface Vessel American Control Conference June -. Portland OR USA FrB. Nonlinear Tracking Control of Underactuated Surface Vessel Wenjie Dong and Yi Guo Abstract We consider in this paper the tracking control problem

More information

Outline. Input to state Stability. Nonlinear Realization. Recall: _ Space. _ Space: Space of all piecewise continuous functions

Outline. Input to state Stability. Nonlinear Realization. Recall: _ Space. _ Space: Space of all piecewise continuous functions Outline Input to state Stability Motivation for Input to State Stability (ISS) ISS Lyapunov function. Stability theorems. M. Sami Fadali Professor EBME University of Nevada, Reno 1 2 Recall: _ Space _

More information

A conjecture on sustained oscillations for a closed-loop heat equation

A conjecture on sustained oscillations for a closed-loop heat equation A conjecture on sustained oscillations for a closed-loop heat equation C.I. Byrnes, D.S. Gilliam Abstract The conjecture in this paper represents an initial step aimed toward understanding and shaping

More information

Nonlinear stabilization via a linear observability

Nonlinear stabilization via a linear observability via a linear observability Kaïs Ammari Department of Mathematics University of Monastir Joint work with Fathia Alabau-Boussouira Collocated feedback stabilization Outline 1 Introduction and main result

More information

Convexity of the Reachable Set of Nonlinear Systems under L 2 Bounded Controls

Convexity of the Reachable Set of Nonlinear Systems under L 2 Bounded Controls 1 1 Convexity of the Reachable Set of Nonlinear Systems under L 2 Bounded Controls B.T.Polyak Institute for Control Science, Moscow, Russia e-mail boris@ipu.rssi.ru Abstract Recently [1, 2] the new convexity

More information

Lyapunov Stability Analysis of a Twisting Based Control Algorithm for Systems with Unmatched Perturbations

Lyapunov Stability Analysis of a Twisting Based Control Algorithm for Systems with Unmatched Perturbations 5th IEEE Conference on Decision and Control and European Control Conference (CDC-ECC) Orlando, FL, USA, December -5, Lyapunov Stability Analysis of a Twisting Based Control Algorithm for Systems with Unmatched

More information

On the representation of switched systems with inputs by perturbed control systems

On the representation of switched systems with inputs by perturbed control systems Nonlinear Analysis 60 (2005) 1111 1150 www.elsevier.com/locate/na On the representation of switched systems with inputs by perturbed control systems J.L. Mancilla-Aguilar a, R. García b, E. Sontag c,,1,

More information

Output Regulation of Uncertain Nonlinear Systems with Nonlinear Exosystems

Output Regulation of Uncertain Nonlinear Systems with Nonlinear Exosystems Output Regulation of Uncertain Nonlinear Systems with Nonlinear Exosystems Zhengtao Ding Manchester School of Engineering, University of Manchester Oxford Road, Manchester M3 9PL, United Kingdom zhengtaoding@manacuk

More information

1 Relative degree and local normal forms

1 Relative degree and local normal forms THE ZERO DYNAMICS OF A NONLINEAR SYSTEM 1 Relative degree and local normal orms The purpose o this Section is to show how single-input single-output nonlinear systems can be locally given, by means o a

More information

VECTOR Lyapunov functions have been used for a long

VECTOR Lyapunov functions have been used for a long 2550 IEEE TRANSACTIONS ON AUTOMATIC CONTROL, VOL 58, NO 10, OCTOBER 2013 Global Stabilization of Nonlinear Systems Based on Vector Control Lyapunov Functions Iasson Karafyllis Zhong-Ping Jiang, Fellow,

More information

Least Squares Based Self-Tuning Control Systems: Supplementary Notes

Least Squares Based Self-Tuning Control Systems: Supplementary Notes Least Squares Based Self-Tuning Control Systems: Supplementary Notes S. Garatti Dip. di Elettronica ed Informazione Politecnico di Milano, piazza L. da Vinci 32, 2133, Milan, Italy. Email: simone.garatti@polimi.it

More information

Lecture 8. Chapter 5: Input-Output Stability Chapter 6: Passivity Chapter 14: Passivity-Based Control. Eugenio Schuster.

Lecture 8. Chapter 5: Input-Output Stability Chapter 6: Passivity Chapter 14: Passivity-Based Control. Eugenio Schuster. Lecture 8 Chapter 5: Input-Output Stability Chapter 6: Passivity Chapter 14: Passivity-Based Control Eugenio Schuster schuster@lehigh.edu Mechanical Engineering and Mechanics Lehigh University Lecture

More information

Nonlinear Control. Nonlinear Control Lecture # 8 Time Varying and Perturbed Systems

Nonlinear Control. Nonlinear Control Lecture # 8 Time Varying and Perturbed Systems Nonlinear Control Lecture # 8 Time Varying and Perturbed Systems Time-varying Systems ẋ = f(t,x) f(t,x) is piecewise continuous in t and locally Lipschitz in x for all t 0 and all x D, (0 D). The origin

More information