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Adaptative high-gain extended Kalman filter and applications

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

Proof.<br />

The first bound of (B.5) gives:<br />

<strong>and</strong> the second is rewritten:<br />

x2(−) ≤ 2b<br />

a<br />

x1(+) ≤ 2b<br />

a<br />

+ 2b<br />

a<br />

+ 2b<br />

a<br />

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

1<br />

e2bτ1 + rτ1,<br />

− 1<br />

x1(+) − 2b<br />

a<br />

x1(+) � e 2b(τ2−τ1) − 1 � + 2b<br />

a<br />

We want to replace x1(+) by the upper bound found above.<br />

Let us define the function<br />

2bxe<br />

h(x) =<br />

2bτ<br />

ax (e2bτ − 1) + 2b .<br />

Its derivative w.r.t. x is<br />

h ′<br />

(x) = e2bτ 2b � ax(e 2bτ − 1) + 2b � − a(e 2bτ − 1)xe 2bτ 2b<br />

[ax(e 2bτ − 1) + 2b] 2<br />

=<br />

e 2bτ (2b) 2<br />

[ax(e 2bτ − 1) + 2b]<br />

It is positive for all τ > 0, <strong>and</strong> we can replace x1(+) by its upper bound:<br />

x2(−) ≤ 2b 2b<br />

+<br />

a a<br />

�<br />

2b 2b 1<br />

a + a e2bτ �<br />

1−1<br />

+ rτ1 − 2b<br />

a<br />

� �e �<br />

1 + rτ1<br />

2b(τ2−τ1) 2b − 1 +<br />

≤ 2b<br />

a<br />

+ 2b<br />

a<br />

� 2b<br />

a<br />

2b<br />

a<br />

+ 2b<br />

a<br />

1<br />

e2bτ1 − 1<br />

e 2bτ 1−1<br />

� 2b<br />

a<br />

+ 2b<br />

a<br />

+ 2b<br />

a<br />

� 2b<br />

a<br />

2 .<br />

1<br />

e2bτ1−1 + 2b<br />

a<br />

1<br />

� �e �<br />

+ rτ1<br />

2b(τ2−τ1) 2b − 1 +<br />

1<br />

e2bτ1−1 We upper bounds the denominator of the last term with:<br />

�<br />

2b 2b 1<br />

+<br />

a a e2bτ1 � �<br />

+ rτ1 e<br />

− 1 2b(τ2−τ1)<br />

�<br />

− 1<br />

<strong>and</strong> the denominator of the second term with:<br />

�<br />

2b 2b 1<br />

+<br />

a a e2bτ1 � �<br />

+ rτ1 e<br />

− 1 2b(τ2−τ1)<br />

�<br />

− 1<br />

We also simplify (2b/a) in those two terms:<br />

x2(−) ≤ 2b<br />

a<br />

≤ 2b<br />

a<br />

+ 2b<br />

a<br />

+ 2b<br />

a<br />

+ 2b<br />

a ≥<br />

� 2b<br />

a<br />

+ 2b<br />

a<br />

.<br />

a<br />

rτ1<br />

� �e � .<br />

+ rτ1<br />

2b(τ2−τ1) 2b − 1 +<br />

+ 2b<br />

a<br />

≥ 2b<br />

a ,<br />

1<br />

e2bτ1 � �<br />

e<br />

− 1<br />

2b(τ2−τ1)<br />

�<br />

− 1 + 2b<br />

a .<br />

1<br />

e2bτ1 1<br />

��<br />

− 1 1+ 1<br />

e2bτ � �e � � + rτ1,<br />

2b(τ2−τ1)<br />

1−1<br />

− 1 +1<br />

1<br />

e2bτ2 − e2bτ1 + e2bτ1 + rτ1.<br />

− 1<br />

138<br />

a<br />

a

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