2016
DOI: 10.1080/17445302.2016.1169632
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Influences of pipe–soil interaction on dynamic behaviour of deepwater S-lay pipeline under random sea states

Abstract: The pipe-soil interactions have an important influence on the dynamic behaviour of offshore pipelines in the touchdown zone (TDZ) during deepwater S-lay. This paper mainly aims to reveal the dynamic behaviour of the pipeline in the TDZ, and its actual dynamic lay effects. A full finite element model for deepwater S-lay systems is primarily developed to simulate the dynamic responses of offshore pipeline from the pipelay vessel via the stinger to the seabed, in which pipelay vessel motions, pipeline hydrodynami… Show more

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Cited by 16 publications
(10 citation statements)
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“…When the lateral displacement y exceeds the range between −ybreakout and +ybreakout, the friction force of the pipe is equal to ) (z P μ , where P(z) is the vertical seabed resistance and μ is the soil friction coefficient. This model could effectively avoid the discontinuous nature of the friction force at zero lateral displacement and was conveniently implemented in the numerical program [30].…”
Section: Pipe-seabed Soil Interactionmentioning
confidence: 99%
See 1 more Smart Citation
“…When the lateral displacement y exceeds the range between −ybreakout and +ybreakout, the friction force of the pipe is equal to ) (z P μ , where P(z) is the vertical seabed resistance and μ is the soil friction coefficient. This model could effectively avoid the discontinuous nature of the friction force at zero lateral displacement and was conveniently implemented in the numerical program [30].…”
Section: Pipe-seabed Soil Interactionmentioning
confidence: 99%
“…When the lateral displacement y exceeds the range between −ybreakout and +ybreakout, the friction force of the pipe is equal to ) (z P μ , where P(z) is the vertical seabed resistance and μ is the soil friction coefficient. This model could effectively avoid the discontinuous nature of the friction force at zero lateral displacement and was conveniently implemented in the numerical program [30]. In another view of the horizontal plane, the lateral and axial pipe-seabed interactions were simulated by the modified Coulomb friction model, which expressed the lateral resistance and axial friction force with the deflection as a bilinear equation, as illustrated in Figure 5.…”
Section: Pipe-seabed Soil Interactionmentioning
confidence: 99%
“…The zerothand first-order terms of k 1 , k 2 , k 3 are given in Equation (A15) in Appendix A2, while the zeroth-and first-order terms of f 1 , f 2 , f 3 are given by Equations ( 23) and (24). Substituting the zeroth-and first-order terms of k 1 , k 2 , k 3 , f 1 , f 2 , f 3 into the six Governing equations and keep only the terms up to first order, we can obtain the first-order Kirchhoff equations as…”
Section: Buckling Analysismentioning
confidence: 99%
“…However, this assumption is typically an oversimplification. For example, a torsional stress can be generated on DNA strands as proteins move along them [1,21]; the flow of intracellular fluid could induce torsional moment on microtubules in cells [22,23]; shear stress is produced due to the anisotropic growth of plant roots [10]; a torsional moment on pipelines on the seabed can also be induced by a lateral current [24]. However, the effects of an ambient elastic medium on the buckling of a rod under pure torsion or combined axial and torsional loading remain poorly understood, as highlighted by the summary of previous works given in Table 1.…”
Section: Introductionmentioning
confidence: 99%
“…Examples are paired-column submersibles (PC Semis) [31][32][33][34][35] and CALM buoys [36][37][38][39]. Orcaflex has also found a notable application in pipeline/hoseline strength assessment [40][41][42] and pipeline installation/laying [43][44][45].…”
Section: Introductionmentioning
confidence: 99%