Difference between revisions of "Template:Finite floating body on the surface frequency domain"
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We assume that the problem is invariant in the <math>y</math> direction. | We assume that the problem is invariant in the <math>y</math> direction. | ||
{{general dock type body equations}} | {{general dock type body equations}} | ||
− | where <math>\alpha = \omega^2</math>. The equation under the | + | where <math>\alpha = \omega^2</math>. The equation under the body consists of |
+ | the kinematic condition | ||
+ | <center> | ||
+ | <math> | ||
+ | \mathrm{i}\omega w = \partial_z \phi,\,\,\, z=0,\,\,-L\leq x\leq L | ||
+ | </math> | ||
+ | <center> | ||
+ | plus the kinematic condition |
Revision as of 21:50, 17 September 2009
We consider the problem of small-amplitude waves which are incident on finite floating body occupying water surface for [math]\displaystyle{ -L\lt x\lt L }[/math]. The submergence of the body is considered negligible. We assume that the problem is invariant in the [math]\displaystyle{ y }[/math] direction.
where [math]\displaystyle{ \alpha = \omega^2 }[/math]. The equation under the body consists of the kinematic condition
[math]\displaystyle{ \mathrm{i}\omega w = \partial_z \phi,\,\,\, z=0,\,\,-L\leq x\leq L }[/math]
plus the kinematic condition