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
[math]\displaystyle{ \zeta(t): \quad \mbox{ambient wave elevation. Regular or random with definitions to be given below}. \, }[/math]
[math]\displaystyle{ \xi_1(t): \quad \mbox{Body surge displacement} \, }[/math]
[math]\displaystyle{ \xi_3(t): \quad \mbox{Body heave displacement} \, }[/math]
[math]\displaystyle{ \xi_4(t): \quad \mbox{Body roll displacement} \, }[/math]

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]