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Adaptative high-gain extended Kalman filter and applications

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tel-00559107, version 1 - 24 Jan 2011<br />

B.1 Bounds on the Riccati Equation<br />

In the same manner as in Lemma 78 we conclude that for all τk ≤ T∗, k ∈ N:<br />

�<br />

|Pk(+)| ≤ |P0| + |Q|<br />

�<br />

e<br />

2s<br />

2sT∗ = 1<br />

.<br />

Therefore Pk(+) ≤ 1<br />

α1 Id, for all τk ≤ T∗, k ∈ N, for all subdivisions {τi}i∈N.<br />

Equivalently, from matrix fact 3.(c): α1Id ≤ Sk(+).<br />

We now proceed with the proof of the second part of this subsection. We need a different<br />

set of tools than the one used in the preceding section. It is a series of lemmas adapted from<br />

[57]. As we will see, in addition to the proof of the existence of a lower bound for S, we also<br />

prove that it is a symmetric positive definite matrix for all times.<br />

Lemma 90<br />

For any λ ∈ R ∗ , any solution S : [0,T[→ Sm (Possibly, T =+∞) of<br />

we have for all τ ∈ [0,T[:<br />

dS<br />

dτ<br />

S(τ) =e−λτ φu(τ, 0)S0φ ′<br />

u(τ, 0)<br />

� τ<br />

+λ<br />

0<br />

α1<br />

= −A′ (τ)S − SA(τ) − SQS,<br />

e −λ(τ−v) �<br />

φu(τ,v) S(v) − S(v)QS(v)<br />

�<br />

φ<br />

λ<br />

′<br />

u(τ,v)dv<br />

where φu(τ,s) is such that: � dφu(τ,s)<br />

dτ = −A ′<br />

(τ)φu(τ,s),<br />

φu(s, s) = Id.<br />

(B.11)<br />

Remark 91<br />

Notice that S(τ) is not λ-dependent. This latter scalar is used only to provide us with a<br />

convenient way to express S(τ).<br />

Proof.<br />

Let us consider an equation of the form<br />

φu(τ,s) denotes the resolvent of the system dx<br />

dτ<br />

d<br />

Λ(τ) =−A′ Λ(τ) − Λ(τ)A + F (τ). (B.12)<br />

dτ<br />

dφu(τ,s)<br />

= −A′ x:<br />

dτ = −A ′<br />

φu(τ,s),<br />

φu(s, s) = Id.<br />

We search for a solution of the formΛ( τ) =φu(τ,s)h(τ)φ ′<br />

u(τ,s).<br />

dΛ<br />

dτ = � d<br />

dτ φu(τ,s) � h(τ)φ ′<br />

�<br />

d<br />

u(τ,s)+φu(τ,s)h(τ) dτ φ′<br />

�<br />

u(τ,s)<br />

= −A ′<br />

φu(τ,s)h(τ)φ ′<br />

u(τ,s) − φu(τ,s)h(τ)φ ′<br />

+φu(τ,s) � d<br />

dτ h(τ)� φ ′<br />

u(τ,s)A(τ)<br />

= −A ′<br />

Λ(τ) − Λ(τ)A + φu(τ,s) � d<br />

dτ h(τ)� φ ′<br />

u(τ,s),<br />

144<br />

+φu(t, s) � d<br />

dτ h(τ)� φ ′<br />

u(τ,s)<br />

u(τ,s)

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