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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Published in | Ocean engineering Vol. 64; pp. 161 - 173 |
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Main Authors | , , , |
Format | Journal Article |
Language | English |
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15.05.2013
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ISSN | 0029-8018 1873-5258 |
DOI | 10.1016/j.oceaneng.2013.01.007 |
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Abstract | 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. |
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AbstractList | 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. |
Author | Amabili, M. Païdoussis, M.P. Epureanu, B.I. Kheiri, M. |
Author_xml | – sequence: 1 givenname: M. surname: Kheiri fullname: Kheiri, M. organization: Department of Mechanical Engineering, McGill University, 817 Sherbrooke Street West, Montreal, QC, Canada H3A 0C3 – sequence: 2 givenname: M.P. surname: Païdoussis fullname: Païdoussis, M.P. email: michael.paidoussis@mcgill.ca organization: Department of Mechanical Engineering, McGill University, 817 Sherbrooke Street West, Montreal, QC, Canada H3A 0C3 – sequence: 3 givenname: M. surname: Amabili fullname: Amabili, M. organization: Department of Mechanical Engineering, McGill University, 817 Sherbrooke Street West, Montreal, QC, Canada H3A 0C3 – sequence: 4 givenname: B.I. surname: Epureanu fullname: Epureanu, B.I. organization: Department of Mechanical Engineering, University of Michigan, Ann Arbor, MI, USA |
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Cites_doi | 10.1017/S002211200600317X 10.1016/0022-460X(76)90598-8 10.1017/S0022112088000540 10.1017/S002211208100075X 10.1115/1.3231213 10.1016/S0022-460X(73)80291-3 10.1061/JYCEAJ.0000873 10.1016/S0022-460X(73)80050-1 10.1016/0898-1221(85)90175-0 10.1017/S0022112068001898 10.1115/1.3448697 10.1016/S0022-460X(75)80051-4 10.1016/S0997-7538(02)01221-4 10.1016/j.jfluidstructs.2005.04.009 10.2514/3.62853 10.1017/S0022112066001484 10.1017/S0022112069002552 |
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Keywords | Flutter Divergence Pinned–pinned pipes Towed pipes Finite difference method Pinned-pinned pipes Equation of motion Towage Numerical simulation Offshore structure Underwater pipe Modeling Axial flow |
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SubjectTerms | Applied sciences Buildings. Public works Divergence Exact sciences and technology Finite difference method Flutter Hydraulic constructions Offshore structure (platforms, tanks, etc.) Pinned–pinned pipes Towed pipes |
Title | Three-dimensional dynamics of long pipes towed underwater. Part 2 Linear dynamics |
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