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- {{sommerfeld radiation condition two dimensions}} {{sommerfeld radiation condition three dimensions}}457 bytes (57 words) - 19:14, 8 February 2010
- {{sommerfeld radiation condition two dimensions}}328 bytes (40 words) - 19:15, 8 February 2010
- ...domain solutions for an incident wave. The theory is present here in two dimensions but can be extended to three dimensions (for plane incident waves) straightforwardly.2 KB (333 words) - 22:32, 29 April 2010
- We show how to solve for the radiation potential for a rigid body and the surrounding fluid in constant [[Finite D {{standard linear wave scattering equations without body condition}}7 KB (1,145 words) - 03:15, 12 February 2010
- {{sommerfeld radiation condition three dimensions}} = Boundary condition at <math>r = a</math> =2 KB (397 words) - 09:33, 20 October 2009
- We must also apply the [[Sommerfeld Radiation Condition]] {{separation of variables in two dimensions}}7 KB (1,297 words) - 08:46, 21 June 2011
- ...vertical plate and determine scattering using [[:Category:Symmetry in Two Dimensions]] must also apply the [[Sommerfeld Radiation Condition]]5 KB (932 words) - 01:23, 7 April 2010
- [[:Category:Symmetry in Two Dimensions|Symmetry in Two Dimensions]].. The full must also apply the [[Sommerfeld Radiation Condition]]4 KB (800 words) - 00:00, 17 October 2009
- There are any situations where we want to expand the three-dimensional linear water wave for the fully three dimensional (depth dependent) case. We begin by assuming the [[Frequency Do7 KB (1,280 words) - 09:34, 20 October 2009
- We must also apply the [[Sommerfeld Radiation Condition]] {{separation of variables in two dimensions}}5 KB (839 words) - 03:37, 28 February 2017
- We must also apply the [[Sommerfeld Radiation Condition]] {{separation of variables in two dimensions}}9 KB (1,520 words) - 01:28, 16 March 2012
- {{sommerfeld radiation condition two dimensions}} We divide the domain into three regions, <math>x<-l</math>,8 KB (1,400 words) - 21:32, 10 February 2010
- ...ons (the main concepts survive almost with no change in the more practical three-dimensional problem). two dimensions. We begin with the equations in the time domian. The simplest problems is [18 KB (2,875 words) - 12:58, 26 April 2011
- The problems consists three regions using [[:Category:Symmetry in Two Dimensions|Symmetry in Two Dimensions]].10 KB (1,978 words) - 23:29, 14 February 2010
- must also apply the [[Sommerfeld Radiation Condition]] ...wikipedia.org/wiki/Separation_of_Variables separation of variables] in the three regions: {<math>x<0 \,</math>},7 KB (1,154 words) - 23:59, 16 October 2009
- must also apply the [[Sommerfeld Radiation Condition]] {{separation of variables in two dimensions}}7 KB (1,111 words) - 00:43, 25 April 2017
- boundary condition applies at the free-surface. It reduced to the [[Free-Surface Green Functio = Two Dimensions =17 KB (2,953 words) - 16:40, 8 December 2009
- ...alpha=\omega^2/g</math> where <math>g</math> is gravity. We also require a condition as <math>\mathbf{x} \to \infty</math> which is the [[Sommerfeld Radiation Condition]]. This depends11 KB (2,041 words) - 08:57, 19 August 2010
- We must also apply the [[Sommerfeld Radiation Condition]] {{separation of variables in two dimensions}}13 KB (2,011 words) - 01:18, 19 March 2012
- {{standard linear wave scattering equations without body condition}} {{sommerfeld radiation condition two dimensions}}14 KB (2,229 words) - 00:26, 25 February 2010