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  • The Free-Surface Green function is one of the most important objects in linear It is based on the [[Frequency Domain Problem]]. The exact form of the Green function
    11 KB (2,041 words) - 08:57, 19 August 2010
  • #REDIRECT [[Free-Surface Green Function for a Floating Elastic Plate]]
    70 bytes (9 words) - 10:16, 30 May 2006
  • This is a special version of the free-surface Green function which applied when the [[Floating Elastic Plate]] ...n Function]] in the limit as the plate terms tend to zero and to the Green function for an infinite plate in the limit as the water terms tend to zero.
    17 KB (2,953 words) - 16:40, 8 December 2009

Page text matches

  • ...H Meylan]], The eigenfunction expansion of the infinite depth free surface Green function in three dimensions, ''Wave Motion'', '''40'''(1),
    1 KB (171 words) - 00:28, 3 August 2006
  • W. D. Kim, On the harmonic oscillations of a rigid body on a free surface, Contains an expression for the [[Free-Surface Green Function]] in [[Infinite Depth]].
    200 bytes (31 words) - 09:44, 29 May 2006
  • A. J. Hermans, Interaction of Free-Surface Waves with Floating Flexible Strips, based on the [[Free-Surface Green Function]]
    283 bytes (38 words) - 09:02, 22 August 2006
  • Contains an expression for the [[Free-Surface Green Function]] in [[Infinite Depth]].
    223 bytes (32 words) - 09:42, 29 May 2006
  • Contains the [[Free-Surface Green Function]] for [[Finite Depth]]
    233 bytes (32 words) - 09:24, 9 December 2006
  • Contains the [[Free-Surface Green Function]] for [[Finite Depth]]
    230 bytes (31 words) - 05:34, 28 April 2009
  • <math>G(x,\xi)</math> is the [[Free-Surface Green Function]] for two-dimensional waves, with singularity at the water surface. We break the surface into <math>N</math> evenly spaced point
    748 bytes (118 words) - 09:06, 19 August 2010
  • It also contain an expression for the [[Free-Surface Green Function]].
    341 bytes (50 words) - 03:54, 1 June 2006
  • using the eigenfunction for the plate and the [[Free-Surface Green Function]]
    292 bytes (41 words) - 08:59, 22 August 2006
  • found by using a special version of the [[Free-Surface Green Function]] which contains the infinite number of image Green functions.
    547 bytes (81 words) - 07:13, 6 July 2006
  • The soluton was found using the [[Free-Surface Green Function]].
    430 bytes (66 words) - 03:02, 10 September 2006
  • on an infinite image system of [[Free-Surface Green Function|Free-Surface Green Functions]] such that <math>z=0</math> coincides with the mean free surface of the water.
    11 KB (1,951 words) - 09:11, 9 January 2009
  • The use of the [[Free-Surface Green Function]] to solve the [[Standard Linear Wave Scattering Problem]] We then use [http://en.wikipedia.org/wiki/Green's_identities Green's second identity]
    2 KB (282 words) - 19:34, 8 February 2010
  • The Free-Surface Green function is one of the most important objects in linear It is based on the [[Frequency Domain Problem]]. The exact form of the Green function
    11 KB (2,041 words) - 08:57, 19 August 2010
  • | previous chapter = [[Solution of Wave-Body Flows, Green's Theorem]] ...xtends easily to flows past ships in calm water and in waves when the free surface condition is more complex than that of the <math>U=0\,</math> frequency dom
    6 KB (949 words) - 23:36, 16 October 2009
  • We consider the entire free surface to be occupied by a [[Floating Elastic Plate]] with a single discontinuity The [[Free-Surface Green Function for a Floating Elastic Plate]] satisfies the following equations (plus the
    18 KB (3,393 words) - 14:11, 6 June 2007
  • using a [[Free-Surface Green Function]] by [[Newman 1994]] and [[Meylan and Squire 1994]]. We describe The simpler problem of dock is treated in [[Green Function Method for Finite Dock]]
    6 KB (980 words) - 10:50, 28 April 2010
  • | chapter title = Solution of Wave-Body Flows, Green's Theorem ...em using either a wave-source potential or the Rankine source as the Green function. The numerical solution of the resulting integral equations in practice is
    13 KB (2,103 words) - 19:55, 26 July 2012
  • This is a special version of the free-surface Green function which applied when the [[Floating Elastic Plate]] ...n Function]] in the limit as the plate terms tend to zero and to the Green function for an infinite plate in the limit as the water terms tend to zero.
    17 KB (2,953 words) - 16:40, 8 December 2009
  • arbitrary geometry in the case of finite depth. Utilising a Green's function they used the standard
    11 KB (1,980 words) - 08:17, 19 October 2009
  • <math>x>r</math>, and <math>-l<x<r</math> so that the body surface is entirely in the an arbitrary continuous function<math>.</math> Our aim is to find the outward normal
    7 KB (1,145 words) - 03:15, 12 February 2010
  • * [[Green Function Methods for Floating Elastic Plates]] ...y [[Squire and Dixon 2000]] and [[Williams and Squire 2002]] using a Green function method applicable to infinitely deep water and they obtained simple express
    7 KB (1,042 words) - 07:15, 4 April 2009
  • Equation (1) is subject to the free edge boundary as a function of arclength <math>s</math> along <math>\partial \Delta</math>;
    9 KB (1,498 words) - 05:48, 30 October 2012
  • <math>x>r</math>, and <math>-l<x<r</math> so that the body surface is entirely in the an arbitrary continuous function<math>.</math> Our aim is to find the outward normal
    8 KB (1,400 words) - 21:32, 10 February 2010
  • This is an generalisation of the [[Dispersion Relation for a Free Surface]], to the case where the surface condition is given by a [[:Category:Floating Elastic Plate|Floating Elastic
    6 KB (1,064 words) - 09:36, 20 October 2009
  • We consider the entire free surface to be occupied by a [[Floating Elastic Plate]] with a single discontinuity = Solution using the [[Free-Surface Green Function for a Floating Elastic Plate]] =
    22 KB (4,078 words) - 05:36, 10 May 2010
  • require the representation of the [[Infinite Depth]], [[Free-Surface Green Function]] immersed surface of body <math>\Delta_j</math>. The source strength distribution
    8 KB (1,256 words) - 08:20, 19 October 2009
  • Denoting the potential at the surface by we introduce the operator <math>\mathbf{G}</math> which maps the surface
    14 KB (2,229 words) - 00:26, 25 February 2010
  • normal derivative of the potential and the potential under the surface of We consider a thin plate, floating on the water surface above a sea bed of
    41 KB (6,389 words) - 09:22, 20 October 2009
  • This results is used to calculate the [[Free-Surface Green Function for a Floating Elastic Plate]]. to show that the function
    20 KB (3,424 words) - 12:02, 11 December 2009
  • one is [[Infinite Array Green Function]] the other is based on appropriate branch of the <math>\arccos</math> function is given by
    14 KB (2,538 words) - 08:21, 19 October 2009
  • Here the ice is treated as a floating material of uniform surface density with no elastic properties nor viscosity. ...de of propagation beneath the raft as compared to that under an open water surface ([[Squire et. al. 1995]]).
    30 KB (4,556 words) - 10:52, 10 September 2009
  • ...roviding a solid barrier between the ocean and atmosphere that hinders the free exchange of heat and moisture between the two. It is also involved in helpi ...reads out across the ocean floor (i.e. away from the poles), rising to the surface because of mixing due to roughness in the sea bed and wind, and returning t
    36 KB (5,801 words) - 09:39, 10 September 2009