Difference between revisions of "Conservation Laws and Boundary Conditions"
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<center><math> \overrightarrow{V} = \nabla \Phi \Rightarrow \nabla \times \nabla \Phi \equiv 0 </math></center> | <center><math> \overrightarrow{V} = \nabla \Phi \Rightarrow \nabla \times \nabla \Phi \equiv 0 </math></center> | ||
− | Where <math>\Phi(X,t)</math> is the velocity potential assumed sufficiently continuously differentiable. | + | Where <math>\Phi(\overrightarrow{X},t)</math> is the velocity potential assumed sufficiently continuously differentiable. |
Potential flow model of surface wave propagation and wave-body interactions very accurate. Few important exceptions will be noted. | Potential flow model of surface wave propagation and wave-body interactions very accurate. Few important exceptions will be noted. |
Revision as of 11:30, 16 January 2007
The Ocean Environment
Non Linear Free-surface Condition
(X,Y,Z): Earth Fixed Coordinate System X: Fixed Eulerian Vector v: Flow Velocity Vector At X
- Free Surface Elevation
Assume ideal fluid (No shear stresses) and irrotational flow:
Let:
Where [math]\displaystyle{ \Phi(\overrightarrow{X},t) }[/math] is the velocity potential assumed sufficiently continuously differentiable.
Potential flow model of surface wave propagation and wave-body interactions very accurate. Few important exceptions will be noted.
Conservation of mass:
or