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Report from Vortex Induced Vibration Specialist Committee of the 25th ITTC

Report from Vortex Induced Vibration Specialist Committee

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Page 1: Report from Vortex Induced Vibration Specialist Committee

Report from Vortex Induced Vibration Specialist Committee of the 25th ITTC

Page 2: Report from Vortex Induced Vibration Specialist Committee

Contents• Members & meetings• Introduction• Review

– Ocean current– Experimental methods– Numerical prediction models

• Assessments• Benchmark bench study• Technical conclusions

Page 3: Report from Vortex Induced Vibration Specialist Committee

Members of the VIV Committee of the 25th ITTC

•Halvor Lie, MARINTEK, Norway (Chairman)

•Elena Ciappy, INSEAN, Italy

•Shan Huang, University of Glasgow & Strathclyde, UK

•Jung-Chun Suh, SNU, Korea

•Xiong-Liang Yao, HEU, China

•Chang-Kyu Rheem, University of Tokyo, Japan

•Don Spencer, Oceanic, Canada

Page 4: Report from Vortex Induced Vibration Specialist Committee

Four committee meetings• INSEAN, Italy, March 2006

• Harbin Engineering University, China, September 2006

• MARINTEK, Trondheim, Norway, October 2007

• University of Tokyo, Japan, February 2008

Page 5: Report from Vortex Induced Vibration Specialist Committee

Recommendation given to the committee1. Conduct an in-depth review of Vortex Induced

Vibration (VIV) and Vortex Induced Motion (VIM), including experimental and numerical modeling. Identify and report on technology gaps and make recommendations for future work.

2. Conduct an assessment of different prediction methods, and make recommendations on their application and limitations.

3. Define and initiate a specific benchmark case study to be used to compare different experimental techniques. This could be based upon existing or new experiments.

Page 6: Report from Vortex Induced Vibration Specialist Committee

Vortex Induced Vibrations

Strouhal frequency: fs = St U / D

Example: Riser with D = 0.3 m, U = 1.5 m/s: fs = 1 Hz, Ts = 1 s

Example: SPAR with D = 30 m, U = 1.5 m/s: fs = 0.01 Hz, Ts = 100 s

Current

In-line oscillations A≈D/4

Vortex shedding

Cross-flow oscillations A≈D

Page 7: Report from Vortex Induced Vibration Specialist Committee

Consequences of VIV

• Risk of fatigue damage

• Increased current drag

Page 8: Report from Vortex Induced Vibration Specialist Committee

VIV problem areas

Page 9: Report from Vortex Induced Vibration Specialist Committee

Strouhal Number vs. Reynolds Number

MS & CFD

FS

Page 10: Report from Vortex Induced Vibration Specialist Committee

Experimental Methods• Two different set-ups

– 2D tests with rigid cylinder with various geometrical shapes that are either elastic mounted, free to move or with forced motion and towed in still water

– 3D test with long elastic cylinder with varying geometries and boundary conditions, free to vibrate. Various flow condition and current profiles may be arranged

Page 11: Report from Vortex Induced Vibration Specialist Committee

Cross-Flow VIV

Behaviour

Page 12: Report from Vortex Induced Vibration Specialist Committee

Lift Coefficient from Forced Motion 2D Test (Gopalkrishnan)

ˆ /oscf f D U=

/A D

Page 13: Report from Vortex Induced Vibration Specialist Committee

Riser eigenmodes

To each mode, n, there corresponds an eigen- frequency, fn . The riser will oscillate when the Strouhal frequency is close to an eigenfrequency:

fn ≈

fs = St⋅U/D

Hence, the speed of the current will determine which mode (n) will respond.

5 10 15 20 25 30 35 40−1

−0.9

−0.8

−0.7

−0.6

−0.5

−0.4

−0.3

−0.2

−0.1

0

n: 1 2 3 4 5 6 7 ....

.....

f1 f2 f3 f4 f5 f6 f7 ....

Page 14: Report from Vortex Induced Vibration Specialist Committee

Complex hydroelastic interactions for long risers in sheared flow

f1 f2 f3 f4 f5 f6

Strouhal Frequencyfs = St U/d

Current profile, URiser

Natural frequencies:

Competing modes

Varying current profile: Many possible frequencies of oscillation exist. ”Competition” between modes. Difficult to predict frequency.

Page 15: Report from Vortex Induced Vibration Specialist Committee
Page 16: Report from Vortex Induced Vibration Specialist Committee

CF and IL fatigue vs. tow speed for bare riser in uniform flow

Page 17: Report from Vortex Induced Vibration Specialist Committee

Max. fatigue damage vs. tow speed

1.00E-11

1.00E-10

1.00E-09

1.00E-08

1.00E-07

1.00E-06

1.00E-05

1.00E-04

1.00E-03

1.00E-02

1.00E-01

1.00E+00

0.00 0.50 1.00 1.50 2.00 2.50

Velocity [m/s]

D [1

/yrs

] Bare17.5D0.25D5D0.14D

Page 18: Report from Vortex Induced Vibration Specialist Committee

Systematic study of triple-start straked risers

-240 -230 -220 -210 -200 -190 -180 -170 -160 -150 -140 -130 -120 -110 -100 -90 -80 -70 -60 -50 -40 -30 -20 -10 0 10 20 30 40 50 60 70 80 90 100 110 120 130 140 150 160 170 180 190 200 210 220 230 2mm-180

-160

-140

-120

-100

-80

-60

-40

-20

0

20

40

60

80

100

120

140

160

mm

-0.250 -0.217 -0.183 -0.150 -0.117 -0.083 -0.050 -0.017 0.017 0.050 0.083 0.117 0.150 0.183 0.217 0.250

Vector map: 3D vectors, 124×96 vectors (11904)Burst#; rec#: 1; 41 (6), Date: 09.02.2005, Time: 02:43:59:185

3D velocity vector plot based on the PIV measurements Arrows present velocity in the paper planeColours the velocity normal to paper plane

Page 19: Report from Vortex Induced Vibration Specialist Committee

Soft marine growth (slimy marine grass)

Soft marine growth on a real riser

Soft marine as a model

Page 20: Report from Vortex Induced Vibration Specialist Committee

Hard marine growth (Shell, wart barnacle, etc.)

Hard marine growth on a real riser

Hard marine growth as modeled

Page 21: Report from Vortex Induced Vibration Specialist Committee

Instability of Faired Riser, 3 D Test

Fairing

Riser

Page 22: Report from Vortex Induced Vibration Specialist Committee

Ocean currents and measurement• High variability of the current presents new

requirements to the way that the ocean currents should be modelled

• Design current profiles are often established based upon field measurements of the current velocities at a number of current meters arranged along a vertical line at the location

• Reliable methods for obtaining design current conditions for a given deep water location have yet to be developed

Page 23: Report from Vortex Induced Vibration Specialist Committee

Semi-empirical VIV models

• Semi-empirical models for VIV response analysis use the hydrodynamic force coefficients such as drag coefficient, lift coefficient, added mass coefficient and hydrodynamic damping coefficient.

• These coefficients are normally obtained from rigid-cylinder model tests with forced motions

Page 24: Report from Vortex Induced Vibration Specialist Committee

Semi-empirical VIV models - Commercial softwareShear7 (MIT)VIVA (MIT)VIVANA (MARINTEK)

Cross-flow oscillations onlyAdequate prediction of response for circular cross sections for low modal cases when exposed to 2D uniform and mildly sheared currentsLarge uncertainties in fatigue, need high SFFurther improvements needed for other cases with non- circular cross sections, higher modal responses (>10th mode) and more complex current profiles

Page 25: Report from Vortex Induced Vibration Specialist Committee

Wake Oscillator Models• Use a van der Pol oscillator to represent the

time-varying force, which is coupled to body motion

• The models generally have the following characteristics– Oscillator is self-exciting and self-limiting– Natural frequency of the oscillator is

proportional to the free stream velocity such that the Strouhal relationship is satisfied

– Cylinder motion interacts with the oscillator

Page 26: Report from Vortex Induced Vibration Specialist Committee

Computational Fluid Dynamics• Stationary cylinder

– Direct Navier Stokes (DNS) for Rn<10000– Large Eddy Simulations (LES)– Reynolds-Averaged Navier-Stokes (RANS)

Page 27: Report from Vortex Induced Vibration Specialist Committee

Computational Fluid Dynamics• Oscillating cylinder

– A certain number of 2D numerical simulations on VIV can be found

– 3D simulations are quite limited and usually refer to low Reynolds number values and small aspect ratio.

– Direct Navier Stokes (DNS)– Large Eddy Simulations (LES)– Reynolds-Averaged Navier-Stokes (RANS)– Discrete Vortex Method (DVM)

Page 28: Report from Vortex Induced Vibration Specialist Committee

Validation of prediction modelsKey results from blind test, Chaplin et al. (2005)

Empirical codesEmpirical codesCFD

Page 29: Report from Vortex Induced Vibration Specialist Committee

Validation of prediction models• Summary of comparison between laboratory measurements

and blind predictions of 11 numerical models, ref. Chaplin et al. (2005)– In general, empirical models were more successful in predicting

CF displacements and curvatures than CFD codes– Big spread of the results regarding CF curvature predictions and

almost all are not conservative– IL displacement is underestimated by all numerical models– IL curvature calculated only by CFD codes but it is in very poor

agreement with the measurements.

Page 30: Report from Vortex Induced Vibration Specialist Committee

Define and initiate a specific benchmark case study

A remaining task, but• OMAE has ongoing activity for benchmarking VIV, where

numerical prediction results will be compared with experimental results

• Suggest that ITTC should establish cooperation with OMAE on the benchmark activity, where ITTC can provide valuable experimental data to OMAE

• Define and initiate a benchmark model test study, where results from various experiments will be compared. The recommended test set-up compromises a rigid cylinder which is elastically mounted and free to move.

Page 31: Report from Vortex Induced Vibration Specialist Committee

Define and initiate a specific benchmark case study

Example of possible test set-up though different test set-ups are permissible

Page 32: Report from Vortex Induced Vibration Specialist Committee

Technical Conclusions– General trends

• Oil and gas industry strong focus on VIV because VIV can be a detrimental factor in offshore field developments with potential huge economic losses and reduced safety, particularly in deep water. Marine risers, free spanning pipelines, tethers and floating vessels are typical structures subjected to VIV

• VIV difficult subject with a complex structural-hydrodynamic interaction. Generally less well understood than other marine loading processes. Considered to be correspondingly less accurate

• During the last decade there has been a great deal of VIV focused research activities, both in the industry and in the academia

Page 33: Report from Vortex Induced Vibration Specialist Committee

Technical Conclusions– Experimental studies

• Important for determination of coefficients used in semi-empirical codes

• Important for verification of numerical methods/studies• Relatively large uncertainties of various parameters (i.e. Rn, 3D

current, IL effect). Their influences on VIV are not well understood

• Most of experiments are done in the sub-critical Rn regime• Lack of data for higher, full-scale Rn regime• Demand for full-scale measured data with coherent high quality

environmental and response data• The experimental results depend on the test set-up, but no

recommendations/guidelines exist

Page 34: Report from Vortex Induced Vibration Specialist Committee

Technical Conclusions– Prediction methods

• CFD still considered as research tool with prohibitive demand for CPU and large uncertainties. However, probably the method yet to realize its potential in the future

• Semi-empirical prediction methods are currently used in the design of marine risers and other slender structures. In the last decade the methods have been improved

– Prediction of response for low modal cases when exposed to 2D uniform and mildly sheared currents appear to be adequate

– For other cases the methods need further improvements– Only the CF VIV response is normally dealt with. Recommended to

incorporate IL response in future models

Page 35: Report from Vortex Induced Vibration Specialist Committee

Suggestion to further activitiesThe ITTC VIV committee suggest to continue its activity

for one more term with the following tasks:

1. Define and initiate a benchmark model test study, where results from various experiments will be compared. The recommended test set-up compromises a rigid cylinder which is elastically mounted and free to move.

2. Recommended that ITTC should establish cooperation with OMAE on the benchmark activity, where ITTC can provide valuable experimental data to OMAE

Page 36: Report from Vortex Induced Vibration Specialist Committee

Suggestion to further activities

2. Evaluate need for guidelines on VIV experiment

3. Evaluate need for defining and standardizing VIV related nomenclatures

4. Update VIV review including assessment of experimental and numerical prediction models and the proposed benchmark study activities of ITTC VIV Committee and OMAE

Page 37: Report from Vortex Induced Vibration Specialist Committee

Thank You