Tayler 1986: Difference between revisions

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280 pp. 1986.
280 pp. 1986.


Contains a description of the [[Floating Elastic Plate]] problem  
Contains a description of the [[Floating Elastic Plate]] problem for a single plate on finite
length in two-dimensions
on [[Infinitely Deep]] water
on [[Infinitely Deep]] water
as a model for a floating breakwater.
as a model for a floating breakwater.
Line 11: Line 12:
to <math>L\,</math> (which can be choosen freely) and time with respect to <math>\sqrt{L/g}\,</math> and the non-dimensional
to <math>L\,</math> (which can be choosen freely) and time with respect to <math>\sqrt{L/g}\,</math> and the non-dimensional
parameters are
parameters are
where <math>\alpha = \omega^2\, </math> </math><math>\beta = D/(\rho g L^4)\,</math>  
where <math>\alpha = \omega^2\, </math><math>\beta = D/(\rho g L^4)\,</math>  
and <math>\gamma = \rho_i h/(\rho L)\,</math>.
and <math>\gamma = \rho_i h/(\rho L)\,</math>.

Revision as of 08:25, 16 May 2006

A. B. Tayler, Mathematical Models in Applied Mathematics, Clarandon Press, 280 pp. 1986.

Contains a description of the Floating Elastic Plate problem for a single plate on finite length in two-dimensions on Infinitely Deep water as a model for a floating breakwater. An approximate solution is the limit of small scattering is presented. The book introduces the non-dimensionalisation in which length is scaled with respect to [math]\displaystyle{ L\, }[/math] (which can be choosen freely) and time with respect to [math]\displaystyle{ \sqrt{L/g}\, }[/math] and the non-dimensional parameters are where [math]\displaystyle{ \alpha = \omega^2\, }[/math][math]\displaystyle{ \beta = D/(\rho g L^4)\, }[/math] and [math]\displaystyle{ \gamma = \rho_i h/(\rho L)\, }[/math].