Proceedings of the ... International Conference on Offshore Mechanics and Arctic Engineering, Volume 5American Society of Mechanical Engineers, 2007 - Arctic regions |
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Page 312
... given by K + V since L is a quadratic form in วน . Using ( 14 ) and ( 15 ) , one finds that ( p1G ( n ) + pG1 ( n ) ... given by Ambrosi [ 9 ] , however the form of the Hamiltonian is to our knowledge new . As in the first case , the ...
... given by K + V since L is a quadratic form in วน . Using ( 14 ) and ( 15 ) , one finds that ( p1G ( n ) + pG1 ( n ) ... given by Ambrosi [ 9 ] , however the form of the Hamiltonian is to our knowledge new . As in the first case , the ...
Page 392
... given wave amplitude A and wave length 2. The Stokes wave solution for the IGN equations are obtained numerically [ 12 ] . When steepness of incoming wave is high , or when reflected wave reaches the inlet boundary , the numerical ...
... given wave amplitude A and wave length 2. The Stokes wave solution for the IGN equations are obtained numerically [ 12 ] . When steepness of incoming wave is high , or when reflected wave reaches the inlet boundary , the numerical ...
Page 521
... given by x = To Toxw x = ToTox + To ( Toxw + Toxw ) x = To Tox + 2T ( Toxw + Tax ) + To ( Toxw + 2Tpxw + Toxw ) ( 5 ) Using equation ( 5 ) , wind load X and gravity load Xw , equation of motion of a blade element is given by 1 ...
... given by x = To Toxw x = ToTox + To ( Toxw + Toxw ) x = To Tox + 2T ( Toxw + Tax ) + To ( Toxw + 2Tpxw + Toxw ) ( 5 ) Using equation ( 5 ) , wind load X and gravity load Xw , equation of motion of a blade element is given by 1 ...
Contents
OCEAN SPACE UTILIZATION | 1 |
OMAE200729521 | 11 |
OMAE200729557 | 17 |
Copyright | |
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26th International Conference aircushion amplitude analysis ASME bathymetry Bay of Fundy beach boundary conditions Bragg scattering breakwater buoy calculated cavitation Coastal coefficient computed Conference on Offshore Copyright 2007 density developed device diameter displacement dynamic effect element equation experimental floating body units flow fluid force frequency function gouge grout hydrodynamic ice load increase installed interaction linear Makran marine maximum measured Mechanics and Arctic method monopile motion mussels nonlinear Ocean ocean energy Offshore Mechanics offshore wind turbine optimization parameters pile pipe pipeline platform pontoon potential predicted pressure problem ratio Research response rotor scale scour depth seabed shown in Figure shrimp significant wave height simulation stray children stress structure Technology tidal power tower tsunami velocity velocity potential vertical Von Mises stress vortex water depth wave energy wave power width wind farms wind speed