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Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed...

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Introduction Stochastic context Illustrative example Structural analysis Conclusion Uncoupled spectral analysis with non-proportional damping N. Blaise, T. Canor & V. Deno¨ el University of Li` ege (Belgium) EACWE 2013 European-African Conference on Wind Engineering July 7-11
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Page 1: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Uncoupled spectral analysiswith non-proportional damping

N. Blaise, T. Canor & V. Denoel

University of Liege (Belgium)

EACWE 2013European-African Conference on Wind Engineering

July 7-11

Page 2: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Introduction

Stochastic context

Illustrative example

Structural analysis

Conclusion

Page 3: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Analysis of structures under random excitations

Structures

are subjected to random excitations

and we have to solve the equation of motion

Page 4: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Dynamic analysis of large structures

Modal basis

Rayleigh Damping

Sources of non-proportionalitydamping devices (TMD, TLCD), aerodynamic damping and...

D is not diagonal

Coupled system of equation of motion

Page 5: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Dynamic analysis of large structures

Modal basis

Rayleigh Damping

Sources of non-proportionalitydamping devices (TMD, TLCD), aerodynamic damping and...

D is not diagonal

Coupled system of equation of motion

Page 6: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Dynamic analysis of large structures

Modal basis

Rayleigh Damping

Sources of non-proportionalitydamping devices (TMD, TLCD), aerodynamic damping and...

D is not diagonal

Coupled system of equation of motion

Page 7: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Dynamic analysis of large structures

Split damping matrix

Decoupling approximation1

Full matrix inversion

1Rayleigh. (1877). The Theory of Sound.Vol. 1. New-York : Dover Publication

Page 8: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Dynamic analysis of large structures

Split damping matrix

Decoupling approximation1

Full matrix inversion

1Rayleigh. (1877). The Theory of Sound.Vol. 1. New-York : Dover Publication

Page 9: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Dynamic analysis of large structures

Split damping matrix

Decoupling approximation1

Full matrix inversion

1Rayleigh. (1877). The Theory of Sound.Vol. 1. New-York : Dover Publication

Page 10: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Asymptotic expansion method

Key-idea1

Approximation of H

1Denoel and Degee. (2009). Asymptotic expansion of slightly coupled modal dynamic transfer functionsnon-proportional damping. Journal of Sound and Vibration 328, 1-2, 1-8

Page 11: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Introduction

Stochastic context

Illustrative example

Structural analysis

Conclusion

Page 12: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Power spectral density matrices

Exact solution

Decoupling approximation

Page 13: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Formulation of the corrections terms

Proposed method1

Corrections terms

1Canor, Blaise and Denoel. (2012). Efficient uncoupled stochastic analysis with non-proportionaldamping. Journal of Sound and Vibration 331, 24, 5283-5291

Page 14: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Formulation of the corrections terms

Proposed method1

Corrections terms

1Canor, Blaise and Denoel. (2012). Efficient uncoupled stochastic analysis with non-proportionaldamping. Journal of Sound and Vibration 331, 24, 5283-5291

Page 15: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Formulation of the corrections terms

Proposed method1

Corrections terms

1Canor, Blaise and Denoel. (2012). Efficient uncoupled stochastic analysis with non-proportionaldamping. Journal of Sound and Vibration 331, 24, 5283-5291

Page 16: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Importance of the corrections terms

Uncorrelated generalized forces - Decoupled solution

First two corrections terms

Page 17: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Importance of the corrections terms

Uncorrelated generalized forces - Decoupled solution

First two corrections terms

Page 18: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Importance of the corrections terms

Uncorrelated generalized forces - Decoupled solution

First two corrections terms

Page 19: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Introduction

Stochastic context

Illustrative example

Structural analysis

Conclusion

Page 20: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Viaduc of Millau

Seven-span cable-stayed bridge (∼2.5 km long)

Crosses the Tarn Valley about 350 m above the river

Finite element model1425 nodes

2439 beam elements with 12 DOFs

Page 21: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Model of wind

Three zones

Main characteristics from on-site measurements

Considering aerodynamic damping r(D) = r(Ds + Da) = 1.02

Page 22: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Modal properties

First 40 modes are kept for the modal analysis (< 1Hz)

Structural modal damping matrix Ds → ξ = 0.3 % in each mode

Page 23: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Introduction

Stochastic context

Illustrative example

Structural analysis

Conclusion

Page 24: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Exact solution

Variances and correlation of modal coordinates

Page 25: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Exact solution

Variances and correlation of modal coordinates

Page 26: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Asymptotic expansion method

Page 27: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Asymptotic expansion method

Variances

Page 28: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Asymptotic expansion method

Correlation of modal coordinates

Page 29: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Introduction

Stochastic context

Illustrative example

Structural analysis

Conclusion

Page 30: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Asymptotic expansion of the modal transfer matrix enables toapproximate a coupled system with non-proportional dampingbased on the decoupled modal transfer matrix Hd

Studied case : Viaduc of MillauSource of non-proportionallity : aerodynamic dampingSecond order approximation of H is sufficient

PerspectivesOrder of approximation function of the frequencyBackground-resonant decomposition for the correction termsDynamic system with non-linear terms

Page 31: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Asymptotic expansion of the modal transfer matrix enables toapproximate a coupled system with non-proportional dampingbased on the decoupled modal transfer matrix Hd

Studied case : Viaduc of MillauSource of non-proportionallity : aerodynamic dampingSecond order approximation of H is sufficient

PerspectivesOrder of approximation function of the frequencyBackground-resonant decomposition for the correction termsDynamic system with non-linear terms

Page 32: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

Asymptotic expansion of the modal transfer matrix enables toapproximate a coupled system with non-proportional dampingbased on the decoupled modal transfer matrix Hd

Studied case : Viaduc of MillauSource of non-proportionallity : aerodynamic dampingSecond order approximation of H is sufficient

PerspectivesOrder of approximation function of the frequencyBackground-resonant decomposition for the correction termsDynamic system with non-linear terms

Page 33: Uncoupled spectral analysis with non-proportional dampingViaduc of Millau Seven-span cable-stayed bridge (˘2.5 km long) Crosses the Tarn Valley about 350 m above the river Finite

Introduction Stochastic context Illustrative example Structural analysis Conclusion

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