Difference between revisions of "Template:Frequency domain equations for the radiation modes"

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\partial_{n}\phi=\mathbf{n}_\nu,\ \ \mathbf{x}\in\partial\Omega_{\mathrm{B}},
 
\partial_{n}\phi=\mathbf{n}_\nu,\ \ \mathbf{x}\in\partial\Omega_{\mathrm{B}},
 
</math></center>
 
</math></center>
where <math>\mathbf{n}_{\nu}</math> is the normal derivative of the <math>\nu</math> mode
+
where <math>\mathbf{n}_{\nu}</math> is the normal derivative of the <math>\nu</math> mode on the
 +
body surface.

Revision as of 09:22, 28 April 2010

The body boundary condition for a radiation mode [math]\displaystyle{ m }[/math] is just

[math]\displaystyle{ \partial_{n}\phi=\mathbf{n}_\nu,\ \ \mathbf{x}\in\partial\Omega_{\mathrm{B}}, }[/math]

where [math]\displaystyle{ \mathbf{n}_{\nu} }[/math] is the normal derivative of the [math]\displaystyle{ \nu }[/math] mode on the body surface.