Applied Sciences
Multiple Timescale Spectral Analysis of Floating Bridges
Margaux Geuzaine
Promoteur : Vincent Denoël
Co-promoteur : Vincent de Ville
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
n
……….…
N
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
n
……….…
N
Distribution statistique
Fréquences relatives
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
n
N
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
Approche statistique
n
……….…
N
Distribution statistique
Fréquences relatives
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
n
N
2
3
3
4
4
4
5
5
5
5
6
6
6
6
7
7
7
7
8
8
8
8
9
9
9
9
10
10
10
11
11
12
7
7
6
8
+
Combinaisons
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
Approche statistique
n
……….…
N
Distribution statistique
Fréquences relatives
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
n
N
2
3
3
4
4
4
5
5
5
5
6
6
6
6
7
7
7
7
8
8
8
8
9
9
9
9
10
10
10
11
11
12
7
7
6
8
+
Combinaisons
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
Approche statistique
n
……….…
N
Distribution statistique
Fréquences relatives
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
n
N
n
N
2
3
3
4
4
4
5
5
5
5
6
6
6
6
7
7
7
7
8
8
8
8
9
9
9
9
10
10
10
11
11
12
7
7
6
8
+
Combinaisons
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
Approche statistique
n
……….…
N
Distribution statistique
Fréquences relatives
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
n
N
n
N
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
P
ro
b
a
b
ilité
d
'o
cc
uren
ce
Distribution de probabilités
n
N
2
3
3
4
4
4
5
5
5
5
6
6
6
6
7
7
7
7
8
8
8
8
9
9
9
9
10
10
10
11
11
12
7
7
6
8
+
Combinaisons
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
Approche probabiliste
Approche statistique
n
……….…
N
Distribution statistique
Fréquences relatives
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
n
N
n
N
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
P
ro
b
a
b
ilité
d
'o
cc
uren
ce
Distribution de probabilités
n
N
2
3
3
4
4
4
5
5
5
5
6
6
6
6
7
7
7
7
8
8
8
8
9
9
9
9
10
10
10
11
11
12
7
7
6
8
+
Combinaisons
3
4
5
6
7
8
9
10
11
12
Somme des dés
2
Simulations
Approche probabiliste
Approche statistique
+ PRÉCIS
+ RAPIDE
+ CLAIR
n
……….…
N
Distribution statistique
Fréquences relatives
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
n
N
n
N
2
3
4
5
6
7
8
9 10 11 12
Somme des dés
1/36
1/18
1/12
1/9
5/36
1/6
P
ro
b
a
b
ilité
d
'o
cc
uren
ce
Distribution de probabilités
n
N
éq. du mouvement
éq. du mouvement
Domaine temporel
Domaine fréquentiel
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<latexit sha1_base64="cBWAQGo6lL1d+TEVEYPa8SErWB0=">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</latexit>
+ théorie des
valeurs extrêmes
éq. du mouvement
Domaine temporel
Domaine fréquentiel
<latexit sha1_base64="wvTFryik02W5qPcDfSOMRnaDfnA=">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</latexit>
<latexit sha1_base64="cBWAQGo6lL1d+TEVEYPa8SErWB0=">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</latexit>
+ théorie des
valeurs extrêmes
éq. du mouvement
Domaine temporel
Domaine fréquentiel
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B
+
R
<latexit sha1_base64="CuM8tcP0KyMtWyvBmGXig8DOUm0=">AAAC13icjVHLSsNAFD3GV62vWJdugkVwVZIi6MJFwY3LCvYhVsskjnVoXkwmUhFxJ279Abf6R+If6F94Z4zgA9EJSc6ce8+Zuff6aSgy5brPY9b4xOTUdGmmPDs3v7BoL1XaWZLLgLeCJExk12cZD0XMW0qokHdTyVnkh7zjD3d0vHPOZSaSeF9dpPwoYoNYnIqAKaL6dqWXiUHE+qPjeo+lqUxG5b5ddWuuWc5P4BWgimI1E/sJPZwgQYAcEThiKMIhGDJ6DuHBRUrcES6Jk4SEiXNcoUzanLI4ZTBih/Qd0O6wYGPaa8/MqAM6JaRXktLBGmkSypOE9WmOiefGWbO/eV8aT323C/r7hVdErMIZsX/pPjL/q9O1KJxiy9QgqKbUMLq6oHDJTVf0zZ1PVSlySInT+ITiknBglB99dowmM7Xr3jITfzGZmtX7oMjN8apvSQP2vo/zJ2jXa55b8/Y2qo3tYtQlrGAV6zTPTTSwiyZa5D3CPR7waB1Y19aNdfueao0VmmV8WdbdG9aVlq4=</latexit>
<latexit sha1_base64="jbxNFiqHEGiK+7+3el/0jNBXPeg=">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</latexit>
éq. du mouvement
Domaine temporel
Domaine fréquentiel
+ théorie des
valeurs extrêmes
<latexit sha1_base64="cBWAQGo6lL1d+TEVEYPa8SErWB0=">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</latexit>
B
+
R
<latexit sha1_base64="CuM8tcP0KyMtWyvBmGXig8DOUm0=">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</latexit>+ RAPIDE
+ CLAIR
- PRÉCIS
<latexit sha1_base64="jbxNFiqHEGiK+7+3el/0jNBXPeg=">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</latexit>éq. du mouvement
Domaine temporel
Domaine fréquentiel
+ théorie des
valeurs extrêmes
<latexit sha1_base64="jbxNFiqHEGiK+7+3el/0jNBXPeg=">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</latexit>
<latexit sha1_base64="EU90pAaQtbOj0qONCGLK44pzdSw=">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</latexit>
Méthode par perturbation pour les intégrales
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
<latexit sha1_base64="jbxNFiqHEGiK+7+3el/0jNBXPeg=">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</latexit>
<latexit sha1_base64="EU90pAaQtbOj0qONCGLK44pzdSw=">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</latexit>
Méthode par perturbation pour les intégrales
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
<latexit sha1_base64="jbxNFiqHEGiK+7+3el/0jNBXPeg=">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</latexit>
<latexit sha1_base64="EU90pAaQtbOj0qONCGLK44pzdSw=">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</latexit>
Méthode par perturbation pour les intégrales
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
Méthode par perturbation pour les intégrales
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2
p
k
2
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B
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
Méthode par perturbation pour les intégrales
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2
p
k
2
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B
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
Méthode par perturbation pour les intégrales
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2
p
k
2
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B
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
Méthode par perturbation pour les intégrales
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2
p
k
2
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B
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
Méthode par perturbation pour les intégrales
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2
p
k
2
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B
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
Méthode par perturbation pour les intégrales
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<latexit sha1_base64="EU90pAaQtbOj0qONCGLK44pzdSw=">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</latexit>
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
BACKGROUND
=
2
p
k
2
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B
=
⇡!
2⇠
S
p
(!)
k
2
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Méthode par perturbation pour les intégrales
=
2
p
k
2
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B
=
⇡!
2⇠
S
p
(!)
k
2
<latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">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</latexit><latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">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</latexit><latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">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</latexit><latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">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</latexit>
R
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
Méthode par perturbation pour les intégrales
Néglige la contribution suivante, ou continue encore...
0
10
-1
5
10
10
2
15
20
10
-2
25
30
10
1
10
-3
10
0
%
=
2
p
k
2
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B
=
⇡!
2⇠
S
p
(!)
k
2
<latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">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</latexit><latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">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</latexit><latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">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</latexit><latexit sha1_base64="YZOrKHzldTG4Y9Z6iMOZcpMkqPI=">AAADDHicjVFPS9xAHH1G659ta7f22EtwKdjLkixCe2hhoQc9WtpVwdhlMs5uh00yYTKRSshX8Jt48yZe/QI9FEHv9Vv4mzFC61LshCRv3u+9N/ObifNEFiYILme82bkn8wuLS62nz54vv2i/XNkuVKm5GHCVKL0bs0IkMhMDI00idnMtWBonYieefLL1nUOhC6myr+YoF/spG2dyJDkzRA3bGx/9aKQZr6JcRoqUNqiKVCrGrK6rXvRD1neCL8N8bUrxtq4m33p1qzVsd4Ju4IY/DcIGdNCMLdX+hQgHUOAokUIggyGcgKGgZw8hAuTE7aMiThOSri5Qo0XeklSCFIzYCX3HNNtr2IzmNrNwbk6rJPRqcvp4Qx5FOk3Yrua7eumSLfuv7Mpl2r0d0T9uslJiDb4T+5jvXvm/PtuLwQjvXQ+SesodY7vjTUrpTsXu3P+jK0MJOXEWH1BdE+bOeX/OvvMUrnd7tszVfzulZe2cN9oSN3aXdMHhw+ucBtu9bhh0w8/rnf6H5qoX8RqrWKP7fIc+NrGFAWWf4CeucO0de6femXd+J/VmGs8r/DW8i1uVBK15</latexit>
R
10
0
10
1
10
2
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1. Repère la contribution principale
2. Introduit une coordonnée étirée appropriée
3. Trouve une approximation locale et intégrable
4. Soustrait-la pour former un nouveau résidu
RESONANTE
processus gaussien
processus non-gaussien
Généralisation aux ordres supérieurs, une nécessité ?
<latexit sha1_base64="cBWAQGo6lL1d+TEVEYPa8SErWB0=">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</latexit>
B
+
R
processus gaussien
processus non-gaussien
Généralisation aux ordres supérieurs, une nécessité ?
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B
+
R
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