Difference between revisions of "Linear Wave-Body Interaction"
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Small wave steepness. Very good assumption for gravity waves in most cases, except when waves are near breaking conditions. | Small wave steepness. Very good assumption for gravity waves in most cases, except when waves are near breaking conditions. | ||
− | * Assume <center><math> \left| \frac{\xi_1}{A} \right| = O(\varepsilon) \ll 1 \, </math><center> | + | * Assume <center><math> \left| \frac{\xi_1}{A} \right| = O(\varepsilon) \ll 1 \, </math></center> |
Revision as of 22:55, 23 February 2007
Linear wave-body interactions
- Consider a plane progressive regular wave interacting with a floating body in two dimensions.
- The main concepts survive almost with no change in the more practical three-dimensional problem
Linear theory
- Assume:
[math]\displaystyle{ \left| \frac{\partial\zeta}{\partial x} \right| = O(\varepsilon) \ll 1 \, }[/math]
Small wave steepness. Very good assumption for gravity waves in most cases, except when waves are near breaking conditions.
- Assume
[math]\displaystyle{ \left| \frac{\xi_1}{A} \right| = O(\varepsilon) \ll 1 \, }[/math]