Difference between revisions of "Template:Incident plane wave"

From WikiWaves
Jump to navigationJump to search
 
Line 7: Line 7:
 
where <math>A</math> is the wave amplitude and <math>k_0</math> is  
 
where <math>A</math> is the wave amplitude and <math>k_0</math> is  
 
the positive imaginary solution of the [[Dispersion Relation for a Free Surface]].
 
the positive imaginary solution of the [[Dispersion Relation for a Free Surface]].
We also have to apply the [[Sommerfeld Radiation Condition]] as <math>\left|\mathbf{r}\right|\rightarrow
 
\infty</math>.
 

Revision as of 07:21, 24 August 2008

The equation is subject to some radiation conditions at infinity. We usually assume that there is an incident wave [math]\displaystyle{ \phi^{\mathrm{{In}}}\, }[/math] is a plane wave travelling in the [math]\displaystyle{ x }[/math] direction

[math]\displaystyle{ \phi^{\mathrm{{In}}}({r},z)=Ae^{k_0 x}\frac{\cos k_0(z+h)}{\cos k_0 h} }[/math]

where [math]\displaystyle{ A }[/math] is the wave amplitude and [math]\displaystyle{ k_0 }[/math] is the positive imaginary solution of the Dispersion Relation for a Free Surface.