Three-dimensional dynamics of long pipes towed underwater. Part 2 Linear dynamics

In this paper, a method of solution based on a finite difference scheme is developed, via which the partial differential equations of motion and boundary conditions, presented in Part 1, are converted into a set of first-order ODEs which are then solved numerically. The mathematical model is validat...

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Bibliographic Details
Published inOcean engineering Vol. 64; pp. 161 - 173
Main Authors Kheiri, M., Païdoussis, M.P., Amabili, M., Epureanu, B.I.
Format Journal Article
LanguageEnglish
Published Kidlington Elsevier Ltd 15.05.2013
Elsevier
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Online AccessGet full text
ISSN0029-8018
1873-5258
DOI10.1016/j.oceaneng.2013.01.007

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Summary:In this paper, a method of solution based on a finite difference scheme is developed, via which the partial differential equations of motion and boundary conditions, presented in Part 1, are converted into a set of first-order ODEs which are then solved numerically. The mathematical model is validated by considering some simplifications which enable us to compare the numerical results with the results of short pipes simply supported at both ends (pinned–pinned) and subjected to axial flow. A typical Argand diagram is then presented for a long pipe (L^=2000m) which shows the evolution of lowest three eigenfrequencies of the system as a function of nondimensional flow velocity (towing speed). For the same pipe, the deformation and time-trace diagrams at different values of flow velocity are also given. The results show clearly that a long pipe towed underwater may lose stability by divergence and at higher flow velocities by flutter; the deformation is confined to a small segment of the pipe, close to the downstream end. Some numerical comparisons are also presented in which the effects of cable stiffness and the skin friction coefficient on the onset of instabilities are studied. ► The present model can be used for both short and long towed pipelines. ► The long pipelines towed underwater may be subject to divergence and flutter. ► For very long pipes the onset of instabilities depends weakly on the pipe length. ► The deformations are confined to a small portion close to the pipe downstream end. ► Increasing the skin friction stabilizes the system but demands more towing power.
ISSN:0029-8018
1873-5258
DOI:10.1016/j.oceaneng.2013.01.007