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1 CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV Riser technology Long term aim: Improve modelling capabilities in RIFLEX in order to make the program more useful for analysis of deep d water systems and marine operations
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Page 1: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

1

CeSOS HighlightsTrondheim 27-29 May 2013

CM Larsen:Slendernstructuresand VIV

Riser technologyLong term aim: Improve modelling capabilities in

RIFLEX in order to make the program more useful for analysis of deep

d water systems and marine operations

Page 2: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

2

Heave compensators; frequent damages

Heave compensation:Ideal model: Integrated hydraulic system and structural dynamics model:

Simulation modelof hydraulic systemas a part of a non-linearFE code for marine riser analysisanalysis

PhD candidate Ausberto Medina

Page 3: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

3

Dynamics of flexible pipes from non-stationary (slug) flow

Riser dynamics Multi-phase flow:Riser dynamics p fTime varying geometryprof. Ole Jørgen Nydal

Direct data communicationHLA / DLL / Total integration

PhD candidate Arturo Ortega

Communication between two independent computer programs:High Level Architecture

Page 4: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

4

Snapshots of flexible riser with slug flow

PhD: Anne Martine RustadCollision between parallel tensioned risers in current

Conventionaltension control:Constant tension,gives different setdown andcollision

Current

Alternativetension control 1:Equal payoutgives different tension which helps, but collision

ill

Alternativetension control 2:Equal effective length (payout + actual riser length)

Carl M. Larsen: Slender structures at DNV, May 2008

collision betweenupstream anddownstream risermay occur

may still take place since different tension will give different length

length)gives parallel risers that do not collide

Page 5: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

5

Steel catenary risers –effective tension and sagbend moment

Bending moment and effective axial forceclose to TDP is strongly influencedby downward axial velocity at upper endby downward axial velocity at upper end

Post doc Elizabeth Passano

Results from non-linear simulations

Corresponding indiv. maxima of ff i i

1400500 m,16.5 m, 16.5 s

14.5 m, 16.0 s

effective tension and bending moment close to TDP, and axial velocity for 500 m depth (grey) and 1800 m depth (coloured) 200

400

600

800

1000

1200

ensi

on (

kN

), m

ax. b

end

ing

mom

ent

(kN

m)

,12.0 m, 15.5 s

1800 m,16.5 m, 16.5 s14.5 m, 16.0 s12.0 m, 15.5 s

Bending moment (kN m)

depth (coloured)

-400

-200

0

-2.5-2-1.5-1-0.5 0

Min

. eff

. t

Min. axial velocity (m/s)Axial velocity (m/s)

Effective axial force (kN)

Page 6: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

6

1200

1400

t (k

Nm

)

16.5 m, 16.5 s14.5 m, 16.0 s12 0 m 15 5 s

Results from non-linear simulations

0

200

400

600

800

1000

ensi

on (

kN

), m

ax. b

end

ing

mom

ent

Max. bending moment

-1.5

8 m

/s

12.0 m, 15.5 sFit

1800 m waterdepth, varyingsignificant wave height and peakperiode

-400

-200

-2.5 -2 -1.5 -1 -0.5 0

Min

. eff

. te

Min. axial velocity (m/s)

Min. effective tension

periode

Est. distEst sample

Sample: 12.0 mSample: 14.5 m

Data from one simulation used to find a functional relation between axial veloccity and response

0.9999

0.9990

0.9900

0.9000

0.5000

0.1000

Pro

bab

ilit

y

Eff. tension Bending moment

pSample: 16.5 m

-200 0 200 400 600 800 1000 1200

Eff. tension (kN), bending. moment (kNm)

Simulated maxima / minima samples for significant wave height 12.0 (blue), 14.5 (light blue) and 16.5 m (red), estimated maxima / minima samples (black) and estimated maxima / minima distributions (grey).

Page 7: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

7

Have we done everything? NO!New techniques for scaled models of deep water floaters

Today's laboratory:D=10m, scale 1:40;400 m water depth

10 m

50 m

400 m water depth

2000 m will requirelaboratory with 50 mwater depth

Alternative method for model tests

Passive springs

Real time computation of forses in slender structures from

Passive springsto obtain correcteigenfrequencies for in-plane motions

structures from measured motions; represent restoring and damping from deep water anchor lines and risers

Forces are adjusted to include dynamics form risers and mooring lines

Page 8: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

8

VIVV VVortex Induced VibrationsLong term aim: Improve empirical analysis tools VIVANA

by developing new experimental techniques and new ways of using data from experiments

Key fetures: Self-limiting, but not a nice, stable responseeven under stationary conditions

Use of supression devices:

Page 9: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

9

We had a workshop 20 years ago

currentprofile

currentprofile

- large differences between results fromcomputer programs

Results 10 years ago

Page 10: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

10

How can VIV be calculated?

• Computational fluid dynamics (CFD)

• Empirical models; based on– data from free oscillation tests

d t f f d ill ti t t

colorful fluid dynamics

– data from forced oscillation tests– data from oscillating flexible beams

• Improvements from CeSOS research

Aronsen's PhD: IL coefficientsForced motion tests

Page 11: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

11

Dynamic IL excitation coefficient and added mass

0 sin( )IL

FC

1st

, 20.5e ILCDLU

21

0, 2 2

0

cos( )

0.25a IL

FC

D L x

3D CFD on VIV

0,25

00.95.6

0.3

1 0

1,5

Present Arosen (2007)

Comparison between CFD and experimentsIn-line forced motions in current (PhD candidate Aronsen)Post doc. Z. Huang

0,2 0,3 0,4 0,5 0,6 0,7 0,8 0,9

0,05

0,10

0,15

0,20

1.02

1.02

1.02

1.02

1.02

1.0

1.0

1.0

1.0

0

0.95

0.95

0

0.9

0.9

0.9

0.9

0.8

0.6

0.8

0.8

0.6

0.6

0.

0.3

0.3

0

0

Am

plit

ud

e r

atio

(A

/D)

Nondimensional frequency

0,2 0,3 0,4 0,5 0,6 0,7 0,8-1,0

-0,5

0,0

0,5

1,0

Ad

ded

mas

s C

a

Nondimensional frequency

Figure 5. Comparison between the numerical results and experimental contour plot of the added mass. The thick line indicates the two excitation regions. ▪, present results.

Page 12: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

12

Kristoffer Aronsen’s PhD:Systematic variation of phase & amplitude

Flowdirection→ →

←← →

510

45

77 90

0.2

0.4

0.6

0.8

1

0.6

0.8

1

[−]

0 45 90 180 225 270

Phase angle, α

→→ →

←←

Carl M. Larsen: Slender structures at DNV, May 2008

05

180185190

225

250 264 0.1 0.15 0.2 0.25 0.30

0.2

0.4

0.6

A/D

[−

Nondimensional frequency [−]

IL and CF forced motions:All data from 300 tests, AIL=0.5 ACF

Hydrodynamic coefficients for combined CF and IL oscillations, all cases

15

Cd

0

5

10

Co

eff

icie

nt

Cd

Ce,cf

Ca,cf

Ce,il

Ca,il

-10

-5

0 0.2 0.4 0.6 0.8 1 1.2

Response amplitude A/D

Page 13: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

13

Data for same phase and relative CF/IL amplitude, varying frequency and A/D

Coefficients for alfa=77, (IL/CF)=0.5

8

-2

0

2

4

6

8

Co

effi

cien

ts (

-)

Ce,cf

Ca,cf

Ce,il

Ca,il

-8

-6

-4

0 0.2 0.4 0.6 0.8 1 1.2

A/D_CF (-)

C

(A/D)CF

Realistic curve, CF oscillation only

All parameters except for amplitude constant

Combined CF and IL oscillation, hydrodyn. coefficientsf_hat = 0.147; A_IL = 0.5 A_CF; phase = 77 deg.

5Ce cf

0

1

2

3

4

n-d

im.

coef

fici

ent

Ce,cfCa,cfCe,il

Ca,ilCd

-3

-2

-1

0 0.2 0.4 0.6 0.8 1 1.2

CF oscillation amplitude (A/D)

No

n

Page 14: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

14

VIVANA: Linear FD analysisAnalysis procedure for structures with local non-linear effects: Kamran Koushan PhD

• Non-linear static analysis• Conventional VIV analysis in frequency domain• Added mass, damping and excitation forces

found• These data are used in a non linear time • These data are used in a non-linear time

domain analysis• NOTE: Only local effects; global response

must be close to the initial response estimate

OMAE 2004

10.0

15.0

20.0

tres

s rm

s (M

Pa)

Linear analysis

Non-linear analysis

Free spanning pipelineNonlinear contact betweenpipe and sea bottom at theshoulders will reduce stresses

0.06

0.08

0.10

nt (

m)

0.02

0.03

0.04

t (m

)

0.0

5.0

0 50 100 150 200 250 300 350 400

Tota

l st

Pipe coordinate (m)

compared to linear analysis

-0.06

-0.04

-0.02

0.00

0.02

0.04

116 120 124 128 132

Pipe coordinate (m)

Dyn

am

ic d

ispl

ace

men

-0.04

-0.03

-0.02

-0.01

0.00

0.01

116 120 124 128 132

Pipe coordinates (m)

Dyn

amic

dis

plac

emen

Page 15: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

15

Database for hydrodynamic coefficients, combined IL and CF response?

o 4 independent variables harmonic IL and CFo 4 independent variables, harmonic IL and CF

o Resolution of 20 values for each variableo 160 000 tests neededo Possible by use of an automatic lab?

o 10 minutes between each runo Takes 3 years!

phasefD

A

D

A

ILCF

ˆ

IL

CF

o Takes 3 years!o 15 values for each parameter requires one yearo But will that be useful?o What about higher order components?

New test technique:Cross section orbits for a flexible beam measured, later used as forced motions for rigid cylinder. Forces measured for the same non-dimensional parameters

10.05 m

10.50

Figure 3: Experimental set-upMeasured forces will include higher order components

Page 16: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

16

Three sets of experiments

Prashant Soni: Uniform flow moderate mode orders tension Uniform flow, moderate mode orders, tension dominated pipe

Ida Aglen:Use of Ormen Lange test data, low mode orders, bending stiffness dominated pipe

Decao Yin: NDP highe mode order tests, mostly tension dominated

Ida Aglen The winner of the first «Researcher Grand Prix»

Page 17: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

17

Prashant Soni (PhD 2008)i:

Results from 250 individual tests,all orbits from uniform flow cases

8

10

CeCF, 1ωCaCF 1ω

0

2

4

6

8

VIV

co

effi

cien

ts (

-)

CaCF, 1ωCeIL, 2ωCaIL, 2ω

Trends?-4

-2

0.125 0.138 0.150 0.163 0.175 0.188 0.200

Non-dimensional frequency (-)

Alternative approach:

Find coefficients directly from flexible beam experiments Jie Wu, PhD

Measure responseMeasure response(strains, accelerations, displacements)

Calculate forces by inverse analysis!y

Supported by Philippe Mainçon

Page 18: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

18

System identification:

Normally we solve a dynamic responseproblem by calculating response from given loadsproblem by calculating response from given loads

Unknown response Knownforces

Question: If we have measured the responseQuestion: If we have measured the response,can we find the forces that must have been there?

Answer: Well, yes – it is possible, but not asstraightforward as you might believe

  Displ. std

80

90

100

New set of curves found from these (and other) results

Excitation Coefficient Database

0 6

0,7

0,8 0

10

20

30

40

50

60

70

80

0 0,002 0,004 0,006 0,008 0,01 0,012 0,014

Displ. (m)

Le

ng

th (

m)

Ce_v1

Displ. modal

Ce_gopal

-0,1

0

0,1

0,2

0,3

0,4

0,5

0,6

0 0,05 0,1 0,15 0,2 0,25 0,3 0,35 0,4

Non-dimensional freq. f_h

Am

pli

tud

e R

atio

A/D

acl0

aclmax

clmax

cla0

Page 19: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

19

Verification 1: Bearman & Chaplin

Spring to limit force variation force variation during a test

Force measurementto control tension

37

to control tensionvariation during a test

Extended comparison:All cases, and both IL and CF response: Dominating mode (frequency) and amplitude show same trends in experiments and calculations

0.3

0.4

0.5

sig/d

ExperimentsVIVANA

0.08

0.1

0.12

0.14

0.16

sig/d

ExperimentsVIVANA

0

0.1

0.2

0 10 20 30 40 50

Red. velocity

0

0.02

0.04

0.06

0 10 20 30 40 50

Red. velocity

Page 20: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

20

0.6

0.8

1

1.2

1.4

A/D

[-]

Series 10

Pure ILCF

IL w/ CFExperiment, CFExperiment, IL

Verification 2:Ormen Lange free spanning pipeline study;CF and IL mode

2.5

3

Series 10

Pure ILCF

IL w/ CFExperiment, CFExperiment, IL

5

6

Series 10

Pure ILCF

IL w/ CFExperiment, CFExperiment IL

0

0.2

0.4

0 0.05 0.1 0.15 0.2 0.25

Current [m/s]

CF and IL mode, frequency and amplitude

0

0.5

1

1.5

2

0 0.05 0.1 0.15 0.2 0.25

Fre

q. [H

z]

Current [m/s]

Experiment, IL

0

1

2

3

4

0 0.05 0.1 0.15 0.2 0.25

Mod

e

Current [m/s]

Experiment, IL

Frequency concert:Concurrent and consecutive response frequencies will have different excitation zones

Combination of frequencies:Concurrent response frequencies, (space sharing)Frequencies act simultaneously, no overlap between excitation zones

min max

Excitationzone for theprimary response frequency; secondeigenfrequency

UC

ˆ 0

c

f Df =

U

5

Mode 3

Combination of frequencies:Consecutive response frequencies, (time sharing )Shift of frequency, full excitation zone when active

5

UC 0ˆc

f Df

Umin max

Excitation zones for each possibleresponse frequency

12

3

4

0.125 0.3

5

Mode 1

5

12

3

4

0.125 0.3

Space sharing vs. Time sharing

Page 21: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

21

Concurrent or consecutive response frequencies:Concurrent will in most cases with shear currentgive more fatigue damage than consecutive

0.08

0.1

0.12

0.14

0.16

0.18

(m)

Response standard deviations

ConcurrentConsecutive

3

4

5

6

7

8

(MPa

)

Srtess standard deviations

ConcurrentConsecutive

g f g g

Response amplitudes Stress std. dev.

0

0.02

0.04

0.06

0 100 200 300 400 500 600 700

Arc length (m)

0

1

2

3

0 100 200 300 400 500 600 700

Arc length (m)

Red: Time sharing Blue: Space sharing

Illustration of the ”frequency concert”in time and space: Both concurrent and consecutive assumptionsrepresent simplifications!

Positi

Freque

Time

ion

ency

Page 22: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

22

One step further:

Philippe Mainçon: Find forces from recent trajectory

L i hiLatest time historyof relative velocitydefines the force!

uIL

FIL(t*), FCF(t*)uCF

TIME DOMAIN VIV MODELING

At each cross sectionapproximate each component of the relative velocityyas a linear combination of n = "15" Laguerre polynomials

Method ensures fine descriptio of recent past, coarse description of further past

0.5

1

1.5x 10

4

y [R

e]

Very fast computation…

0 0.5 1 1.5 2 2.5

x 104

-1.5

-1

-0.5

0

x-velocity [Re]

y-ve

loci

ty

Page 23: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

23

Promising results so far!

What is the potential?• Integrated CF and IL response in time domain!• Higher order force and response components

directly pesent!

• But: We are at present far from a general model

• Need a large data base of trajectories• Data based on our forced motion tests with

measured trajectories is available

Thank you for your y yattention!

Page 24: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

Reference list, Slender marine structures; Carl M. Larsen PhD thesis – Kjetil Skaugset (2003): On suppression of VIV of circular cylinders by radial water jets – Kristoffer Aronsen (2007): An experimental investigation of IL and combined IL-CF VIV – Anne Marthine Rustad (2007): Modeling and control of top tensioned risers – Prashant Soni (2008): Hydrodynamic coefficients for VIV of flexible beams – Jie EWu (2011): Hydrodynamic force identification from stochastic VIV experiments with slender beams – Decao Yin (2013): Experimental and numerical analysis of combined IL and CF VIV

Journal papers /1/ Skaugset, K.B. and Larsen, C.M.:”DNS and experimental investigation on vortex shedding and VIV

modification using radial water jets along circular cylinders”, Journal of Fluid and Structures (Paper accepted for publication 2004)

/2/ Leira, B.J., Sørensen, A.J. and Larsen, C.M.: “A reliability-based control algorithm for dynamic positioning of floating vessels”. Journal of Structural Safety, Vol 26, 2004, pp 1-28

/3/ J R Chaplin, P W Bearman, Y. Cheng, E Fontaine, J.M.R. Graham, K Herfjord, F.J. Huarte, M Isherwood, K. Lambrakos, C M Larsen, J R Meneghini, G Moe, R.J. Pattenden, M S Triantafyllou, R.H.J. Willden: "Blind predictions of laboratory measurements of vortex-induced vibrations of a Tension Riser". Journal of fluid and structures 21 (2005), 25-40

/4/ Baarholm, Gro S., Larsen, C.M. and Lie, Halvor: "On fatigue damage accumulation from in-line and cross-flow vortex induced vibrations on risers" Journal of Fluids and Structures, 22 (2006) 109-127

/5/ Baarholm, Gro S., Larsen, Carl M. and Lie, Halvor: "Reduction of VIV using suppression devices – A Theoretical Approach" Journal of Marine Structures 2006 /6/ Rustad, A. M., Larsen, C. M. and Sørensen, A. J. FEM modelling and automatic control for collision

prevention of top tensioned risers. Marine Structures, 2008, Vol. 21, No. 1, pp. 80-112. /7/ Huang, Z. Y. and Larsen, C. M. Large eddy simulation on interaction between in‐line and crow‐flow

oscillation of a circular cylinder China Ocean Engineering 24(4)

Invited key note lectures /1/ Larsen, C. M. and Lie, H.: On Hydrodynamic Coefficients for Combined Cross-Flow and In-Line Vortex

Induced Vibrations. 27th International Conference of Offshore Mechanics and Arctic Engineering, OMAE 200857569, 15 p., 2008, 15-20 June, Estoril, Portugal.

/2/ Larsen, C. M.: Slender marine structures - key features and methods for design analysis. The 1st International Conference on Sustainable Infrastructure and Built Environment (SIBE), 2009, 2-3 Nov. - Bandung, Indonesia.

/3/ Larsen, C.M., Passano, E. and Lie, H.: Recent development of the empirical basis for prediction of vortex induced vibrations, The 2nd International Conference on Sustainable Infrastructure and Built Environment (SIBE), 2012, 12-13 Nov. - Bandung, Indonesia.

Conference papers /1/ Skaugset, K. and Larsen, C.M.: “Drag force reduction and VIV suppression of circular cylinders using

radial water jets”, OMAE2003-37102, , 22nd International Conference on Offshore Mechanics and Arctic Engineering, June 2003, Cancun, Mexico

/2/ Yttervik, R., Reinholdtsen, S-S, Larsen, C.M. and Furnes, G.K.: ”Marine operations in deep water and a variable current flow environment”. 3rd International Conference on Hydroelasticity in Marine Technology, September 2003, Oxford, UK

/3/ Larsen, Carl M., Baarholm, Gro S., Passano, Elizabeth and Koushan, Kamran: "Non-Linear Time Domain Analysis of Vortex Induced Vibrations for Free Spanning Pipelines" [OMAE2004-51404] Proceedings of 23rd International Conference on Offshore Mechanics and Arctic Engineering, Vancouver, Canada, June 2004

/4/ Soni, P. and Larsen, C. M. "Dynamic Interaction Between Spans in a Multi Span Pipeline Subjected to Vortex Induced Vibrations", OMAE2005-67192, 24th International Conference on Offshore Mechanics and Arctic Engineering, 12-17 June 2005, Halkidiki, Greece

/5/ Larsen, C.M., Baarholm, G.S. and Lie, H: "Influence From Helical Strakes on Vortex Induced Vibrations and Static Deflection of Drilling Risers" OMAE2005-67192. 24th International Conference on Offshore Mechanics and Arctic Engineering, 12-17 June 2005, Halkidiki, Greece

Page 25: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

/6/ Aronsen, K:, Larsen, C.M. and Mørk, K.: " Hydrodynamic Coefficients From In-Line VIV Experiments" OMAE2005-67393, OMAE2005-67192. 24th International Conference on Offshore Mechanics and Arctic Engineering, 12-17 June 2005, Halkidiki, Greece

/7/ Larsen, C.M. and Koushan, K.: " Empirical model for the analysis of vortex induced vibrations of free spanning pipelines" Eurodyn, Paris 2005

/8/ Larsen, C.M. and Passano, E.: "Time and frequency domain analysis of catenary risers subjected to vortex induced vibrations" OMAE 2006-92149, Hamburg

/9/ Passano, E. and Larsen, C.M.: "Efficient analysis of a catenary riser" OMAE 2006-92308, Hamburg /10/ Baarholm, G.S., Larsen, C.M. and Lie, H.: "Effect of strakes on fatigue damage due to cross-flow VIV"

3rd International conference on hydroelastisity in marine technology, Wuxi 2006 /11/ Lie, H. and Larsen, C.M.: "Vortex induced vibrations of deepwater risers and pipelines - review of model

test results" 3rd International conference on hydroelastisity in marine technology, Wuxi 2006 /12/ Soni, P.K. and Larsen, C.M.: "An experimental investigation of interaction between adjacent spans in

pipelines" 3rd International conference on hydroelastisity in marine technology, Wuxi 2006 /13/ Rustad, A. M., C. M. Larsen and A. J. Sørensen (2007). Deep Water Riser Collision Avoidance by

Top Tension Control. In Proc. OMAE, 26th International Conference on Offshore Mechanics and Arctic Engineering, OMAE2007-29172, June 10-15, San Diego, California, USA.

/14/ Rustad, A. M., A. J. Sørensen and C. M. Larsen (2007). Supervisory Switched Control of Marine Risers. In Proceedings of the 7th IFAC Conference on Control Applications in Marine Systems (CAMS2007), September 19-21, Bol, Croatia.

/15/ Anne M. Rustad, Carl M. Larsen, Asgeir J. Sorensen Deep Water Riser Collision Avoidance by Top Tension Control. PAPER: OMAE2007-29172 /16/ Ioannis K. Chatjigeorgiou, Elizabeth Passano, Carl M. Larsen Extreme Bending Moments on Long Catenary Risers Due to Heave Excitation, PAPER: OMAE2007-29384 /17/ Elizabeth Passano; Carl M. Larsen Estimating Distributions for Extreme Response of a Catenary Riser. PAPER: OMAE2007-29547 /18/ Jie Wu, Carl M. Larsen Hydrodynamic Force Identification From Vortex Induced Vibration Experiments With Slender Beams. PAPER: OMAE2007-29174 /19/ Prashant K. Soni, Carl M. Larsen, Chittiappa Muthanna Vortex Induced Vibration of a Rigid Cylinder Oscillating With a Given Trajectory Profile, PAPER: OMAE2007-29193 /20/ Djoni E. Sidarta, Kostas F. Lambrakos; Carl M. Larsen Hydrodynamic Coefficients for Riser In-Line VIV in Sheared Currents. PAPER: OMAE2007-29519 /21/ Kristoffer H. Aronsen; Carl Martin Larsen Hydrodynamic Coefficients for In-Line Vortex Induced Vibrations, PAPER: OMAE2007-29531 /22/ Carl M. Larsen; Rune Yttervik; Kristoffer Aronsen Calculation of In-Line Vortex Induced Vibrations of Free Spanning Pipelines, PAPER: OMAE2007-29533 /23/ Lie, H., Larsen, C. M. and Kaasen, K. E. Frequency domain model for prediction of stochastic vortex

induced vibrations for deep water risers. Proceedings of the 27th International Conference on Offshore Mechanics and Arctic Engineering, OMAE2008-57566, 2008, 15-20 June - Estoril, Portugal.

/24/ Rustad, A. M. and Larsen, C. M. Collision prevention of two different top tensioned risers by automatic control. Proceedings of the 27th International Conference on Offshore Mechanics and Arctic Engineering, OMAE2008-57496, 2008, 15-20 June - Estoril, Portugal.

/25/ Soni, P. K. and Larsen, C. M. Investigating the relevance of strip-theory for pipelines subjected to vortex-induced vibrations. Proceedings of the 27th International Conference on Offshore Mechanics and Arctic Engineering, OMAE2008-57551, 2008, 15-20 June - Estoril, Portugal.

/56/ Swithenbank, S. and Larsen, C. M. The importance of mode number on in-line amplitude of vortex-induced vibrations of flexible cylinders. Proceedings of the 27th International Conference on Offshore Mechanics and Arctic Engineering, OMAE2008-57531, 2008, 15-20 June - Estoril, Portugal.

/27/ Swithenbank, S., Larsen, C. M., Vandiver, J. K. and Lie, H. Reynolds number dependence of flexible VIV response data. Proceedings of the 27th International Conference on Offshore Mechanics and Arctic Engineering, OMAE2008-57045, 2008, 15-20 June - Estoril, Portugal.

/28/ Wu, J., Larsen, C. M. and Kaasen, K. E. A new approach for identification of forces on slender beams subjected to vortex-induced vibrations. Proceedings of the 27th International Conference on Offshore Mechanics and Arctic Engineering, OMAE2008-57550, 2008, 15-20 June - Estoril, Portugal.

/29/ Mainçon, P., Barnardo, C. and Larsen, C.M. (2008): “VIV force estimation using inverse FEM”, OMAE 2008-57375, Estoril, Portugal

/30/ Larsen, C.M. and Lie, H. (2008) “On hydrodynamic coefficients for combined cross-flow and in-line vortex indiced vibrations”, OMAE 2008-57569, Estoril, Portugal

Page 26: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

/31/ Aglen, I., Larsen, C. M. and Nielsen, F. G. Characterization of Measured VIV for Free Spanning Pipelines. OMAE2009, Proceedings of the 28th International Conference on Ocean, Offshore and Arctic Engineering. OMAE2009-79561, 2009, May 31-June 5 - Honolulu (HA), USA.

/32/ Huang, Z. Y., Larsen, C. M. and Cui, W.C. 3-D LES study on a forced oscillating circular cylinder following the figure of eight movement. Proceedings of the Conference on Hydroelasticity in Marine Technology, 2009, 8-10 Sept. - Southampton, UK.

/33/ Soni, P. K. and Larsen, C. M. Vortex Pattern Comparison for Periodic and Harmonic Combined Cross-Flow & In-Line Forced Oscillations. OMAE2009, Proceedings of the 28th International Conference on Ocean, Offshore and Arctic Engineering. OMAE2009-80089, 2009, May 31-June 5 - Honolulu (HA), USA

/34/ Soni, P. K., Larsen, C. M. and Wu, J. Hydrodynamic Coefficients for Vortex Induced Vibrations on Slender Beams. OMAE2009, Proceedings of the 28th International Conference on Ocean, Offshore and Arctic Engineering. OMAE2009-79797, 2009, May 31-June 5 - Honolulu (HA), USA.

/35/ Szwalek, J. and Larsen, C. M. Reynolds Number Effects on Hydrodynamic Coefficients for Pure In-Line and Pure Cross-Flow Vortex Induced Vibrations. OMAE2009, Proceedings of the 28th International Conference on Ocean, Offshore and Arctic Engineering. OMAE2009-79399, 2009, May 31-June 5 - Honolulu (HA), USA.

/36/ Wu, J., Larsen, C. M., Lie, H., Passano, E. and Kendon, T. E. Prediction of Fatigue Damage from Stochastic Vortex Induced Vibrations. Proceedings of the Conference on Hydroelasticity in Marine Technology, 2009, 8-10 Sept. - Southampton, UK..

/37/ Wu, J., Mainçon, P., Larsen, C. M. and Lie, H. VIV Force Identification Using Classical Optimal Control Algorithm. OMAE2009, Proceedings of the 28th International Conference on Ocean, Offshore and Arctic Engineering. OMAE2009-79568, 2009, May 31-June 5 - Honolulu (HA), USA.

/38/ Huang, Z. Y., and Larsen, C. M. A Numerical Study on Vortex Induced Forces and Wake Structures of an Oscillating Cylinder. BBVIV-6. The 6th IUTAM Symposium on Bluff Body Wakes and Vortex-Induced Vibrations. June 22-25, 2010, Capri Island, Italy.

/39/ Larsen, C.M., Aronsen, K. and Soni, P.: "On empirical models for higher order frequency components of vortex induced vibrations", BBVIV-6. The 6th IUTAM Symposium on Bluff Body Wakes and Vortex-Induced Vibrations. June 22-25, 2010, Capri Island, Italy.

/40/ Huang, Z., and Larsen, C. M. Large Eddy Simulation of an Oscillating Cylinder Close to a Wall Proceedings of the 29th International Conference on Ocean, Offshore and Arctic Engineering June 6-11, 2010. Shanghai, China. OMAE2010-20006

/41/ Larsen, C. M., Wu, J., and Lie, H.: On the Understanding of Non-Stationary VIV of Slender Beams. Proceedings of the 29th International Conference on Ocean, Offshore and Arctic Engineering June 6-11, 2010. Shanghai, China. OMAE2010-20348

/42/ Passano, E., Larsen, C. M. and Wu, J. VIV of free spanning pipelines: Comparison of response from a semi-empirical code to model tests Proceedings of the 29th International Conference on Ocean, Offshore and Arctic Engineering June 6-11, 2010. Shanghai, China OMAE 2010-20330

/43/ Soni, P.K. and Larsen, C. M. Response of pipelines under VIV, an experimental investigation Proceedings of the 29th International Conference on Ocean, Offshore and Arctic Engineering June 6-11, 2010. Shanghai, China. OMAE2010-20675

/44/ Sten, R., Hansen, M.R., Saevik, S. and Larsen, C. M. Force Variations in Heave Compensating System for Ultra Deep Water Drilling Risers Proceedings of the 29th International Conference on Ocean, Offshore and Arctic Engineering June 6-11, 2010. Shanghai, China OMAE 2010-20011

/45/ Wu, J. Larsen, C. M. and Lie, H. Estimation of Hydrodynamic Coefficients for VIV of Slender Beam at High Mode Orders Proceedings of the 29th International Conference on Ocean, Offshore and Arctic Engineering June 6-11, 2010. Shanghai, China OMAE 2010-20327

/46/ Yin, D. and Larsen, C. M.: On Determination of VIV coefficients under shear flow condition, Proceedings of the 29th International Conference on Offshore Mechanics and Arctic Engineering. (OMAE 2010-20306). 6-11 June 2010, Shanghai, China.

/47/ Aglen, I.M. and Larsen, C.M.: Importance of Added Mass for the Interaction between IL and CF Vibrations of Free Spanning Pipelines (OMAE2011-49966). Proceedings of the 30th International Conference on Ocean, Offshore and Arctic Engineering. June 19-24, 2011 - Rotterdam, The Netherlands.

/48/ Huang, Z. and Larsen, C. M.: Numerical Simulation on Vortex-Induced Vibration of an Elastically Mounted Circular Cylinder with Two Degrees of Freedom (OMAE2011-49573). Proceedings of the 30th International Conference on Ocean, Offshore and Arctic Engineering, June 19-24, 2011 - Rotterdam, The Netherlands

/49/ Mainçon, P. and Larsen, C. M.: Towards a Time-Domain Finite Element Analysis of Vortex Induced Vibrations (OMAE2011-49539). Proceedings of the 30th International Conference on Ocean, Offshore and Arctic Engineering, June 19-24, 2011 - Rotterdam, The Netherlands.

Page 27: CeSOS Highlights - NTNU M. Larsen.pdf · CeSOS Highlights Trondheim 27-29 May 2013 CM Larsen: Slender structures and VIV ... max. bending momen Max. bending moment-1.58 m/s 12.0 m,

/50/ Yin, D. and Larsen, C. M.: Experimental and Numerical Analysis of Forced Motion of a Circular Cylinder (OMAE2011-49438). Proceedings of the 30th International Conference on Ocean, Offshore and Arctic Engineering, June 19-24, 2011 - Rotterdam, Netherlands

/51/ Larsen, C.M., Zhao, Z. and Lie, H. (2012): “Frequency components of vortex induced vibrations in sheared current”, OMAE2012-83092, Rio de Janeiro, Brazil

/52/ Yin, D. and Larsen, C.M. (2012): “Forced motion experiments with measured motions from flexible beam tests under uniform and sheared flows”, OMAE2012-83160, Rio de Janeiro, Brazil

/53/ Passano, E., Larsen, C.M. and Lie, H. (2012): “Comparison of calculated in-line vortex induced vibrations to model tests”, OMAE2012-83387, Rio de Janeiro, Brazil

/54/ Ortega, A., Rivera, A., Nydal, O.J. and Larsen, C.M.: On the Dynamic Response of Flexible Risers Caused by Internal Slug Flow (OMAE2012-83316). Proceedings of the 31st International Conference on Ocean, Offshore and Arctic Engineering (OMAE2012). 1-6 July 2012 - Rio de Janeiro, Brazil

/55/ Swithenbank, S.B. and Larsen, C.M. (2012): “Occurrence of high amplitude VIV with time sharing”, OMAE2012-83431, Rio de Janeiro, Brazil

/56/ Rustad, A.M., Ervik, A.K., Sørensen, A.J. and Larsen, C.M. Increasing the Operation Window for Drilling Risers on DP Vessels by Monitoring Riser Angles (OMAE2012-83922). Proceedings of the 31st International Conference on Ocean, Offshore and Arctic Engineering (OMAE2012). 1-6 July 2012 - Rio de Janeiro, Brazil.

/57/ Larsen, C.M., Passano, E. and Lie, H.: Recent development of the empirical basis for prediction of vortex induced vibrations, Proceedings of the of the International Conference on Hydroelastisity in Marine Technology 2012 Tokyo, JAPAN


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