vortex-induced waves along cables - École polytechnique

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Vortex-induced Vortex-induced waves waves along along cables cables Matteo Luca FACCHINETTI (1,2) , Emmanuel de LANGRE (1) , Francis BIOLLEY (2) (1) LadHyX – CNRS – Ecole Polytechnique (Paris) - FRANCE (2) Institut Français du Pétrole VORTEX-INDUCED VIBRATIONS DEEPWATER OIL FIELDS q S z y T z t y m = + ˜ ¯ ˆ Á Ë Ê - ... 2 2 ( ) 2 2 2 2 2 3 2 2 2 2 1 t y F z q z t q q t q q t q f f = - - + - + c n w ew FLUID MODEL STRUCTURE MODEL • q = near wake variable ~ fluid lift • spanwise interactions [2] • coupled by the structure acceleration [3] • y = transverse displacement • coupled by the fluid lift Strouhal law w structure dispersion relation k cable c m T k = = w * experimental data model prediction [Dowling (1988)] EXPERIMENTS THEORY Strouhal w w = * experimental data St(Re) law [Williamson (1998)] wave features established by dispersion relations intersection [5] Strouhal w w = cable c m T k = = w evidence of a travelling wave propagating downstream [1] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Vortex-induced waves along a cable ». Proceedings of the 2001 DFD Meeting of The American Physical Society (APS). [2] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Vortex shedding modeling using diffusive van der Pol oscillators ». Comptes Rendus Mécanique, 330 : 451-456, 2002. [3] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « On wake oscillator models for 2-D vortex- induced vibrations ». Journal of Fluids and Structures, submitted for publication, 2002. [4] FACCHINETTI, M.L. & DE LANGRE, E. & FONTAINE, E & BONNET, P.A. & ETIENNE, S. & BIOLLEY, F . « VIV of two cylinders in tandem arrangement: analytical and numerical modeling ». Proceedings of the 2002 International Offshore and Polar Engineering Conference (ISOPE), paper 2002- JRC-05-3-14. [5] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Vortex-induced waves along cables ». Proceedings of the 2002 ASME International Mechanical Engineering Congress, paper IMECE-2002- 32161. [6] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Experiments on vortex-induced waves along cables ». Proceedings of the 2002 Conference on Bluff Body Wakes and Vortex-Induced Vibrations (BBVIV). REFERENCES free-hanging cable in water towing tank [6] • slender structure L/D>10 3 • catenary geometry • non-linear wave reflection focusing on travelling waves fluid w Strouhal structure w s w Strouhal = w s lock-in Vortex shedding has a characteristic frequency defined by the Strouhal number. As it approaches a structure frequency a lock-in occurs and this resonance leads to larger vibration amplitudes. Vortex-Induced Vibrations (VIV) are a major cause of fatigue damage for all structures connecting the well heads at the sea bottom to the floating facilities LadHyX LadHyX The numerical simulation of the entire flow field using the Navier- Stokes equations is not effective because of strong computational requirements. Conversely, a phenomenological wake oscillator model (van der Pol) is proven really useful ... The classical mono-dimensional cable model is effective in describing the main features of the structure dynamics. However, results of the theory extends to more general cases like beams with internal flow … COMPARISON

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Vortex-inducedVortex-induced waveswaves alongalong cablescablesMatteo Luca FACCHINETTI(1,2), Emmanuel de LANGRE(1), Francis BIOLLEY(2)

(1) LadHyX – CNRS – Ecole Polytechnique (Paris) - FRANCE (2) Institut Français du Pétrole

VORTEX-INDUCED VIBRATIONS DEEPWATER OIL FIELDS

qSz

yT

zt

ym =+˜

¯

ˆÁË

Ê∂

∂-

∂...

2

2

( )2

2

2

2

2

322

2

2

1t

yF

z

q

zt

qq

t

qq

t

qff ∂

∂=

∂-

∂∂

∂-+

∂-+

∂cnwewFLUID MODEL STRUCTURE MODEL

• q = near wake variable ~ fluid lift

• spanwise interactions [2]

• coupled by the structure acceleration [3]

• y = transverse displacement

• coupled by the fluid lift

Strouhal law w

structure dispersion relationk

cablecm

T

k==

w

* experimental data

model prediction[Dowling (1988)]

EXPERIMENTSTHEORY

Strouhalww =

* experimental data

St(Re) law[Williamson (1998)]

wave features established by

dispersion relations intersection [5]

Strouhalww =

cablecm

T

k==

w

evidence of a travellingwave propagating

downstream

[1] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Vortex-induced waves along a cable ».Proceedings of the 2001 DFD Meeting of The American Physical Society (APS).

[2] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Vortex shedding modeling using diffusivevan der Pol oscillators ». Comptes Rendus Mécanique, 330 : 451-456, 2002.

[3] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « On wake oscillator models for 2-D vortex-induced vibrations ». Journal of Fluids and Structures, submitted for publication, 2002.

[4] FACCHINETTI, M.L. & DE LANGRE, E. & FONTAINE, E & BONNET, P.A. & ETIENNE, S. &BIOLLEY, F . « VIV of two cylinders in tandem arrangement: analytica l and numerical modeling ».Proceedings of the 2002 International Offshore and Polar Engineering Conference (ISOPE), paper 2002-JRC-05-3-14.

[5] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Vortex-induced waves along cables ».Proceedings of the 2002 ASME International Mechanical Engineering Congress, paper IMECE-2002-32161.

[6] FACCHINETTI, M.L. & DE LANGRE, E. & BIOLLEY, F. « Experiments on vortex-induced wavesalong cables ». Proceedings of the 2002 Conference on Bluff Body Wakes and Vortex-Induced Vibrations(BBVIV).

REFERENCES

free-hanging cable

in water towing tank [6]

• slender structure L/D>103

• catenary geometry

• non-linear wave reflection

focusing on

travelling waves

fluid wStrouhal structure ws

w Strouhal = ws ! lock-in

Vortex shedding has a characteristic frequency defined by theStrouhal number. As it approaches a structure frequency a lock-inoccurs and this resonance leads to larger vibration amplitudes.

Vortex-Induced Vibrations (VIV) are a major cause of fatiguedamage for all structures connecting the well heads at the sea bottomto the floating facilities

LadHyXLadHyX

The numerical simulation of the entire flow field using the Navier-Stokes equations is not effective because of strong computationalrequirements. Conversely, a phenomenological wake oscillatormodel (van der Pol) is proven really useful ...

The classical mono-dimensional cable model is effective indescribing the main features of the structure dynamics. However,results of the theory extends to more general cases like beams withinternal flow …

COMPARISON