Template:Standard linear wave scattering equations without body condition: Difference between revisions
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(note that the last expression can be obtained from combining the expressions: | (note that the last expression can be obtained from combining the expressions: | ||
<center><math> | <center><math> | ||
\partial_z \phi =\mathrm{i} \omega \zeta,\,z=0,\,\,\mathbf{x} \in \partial \Omega_{\mathrm{F}}, | \partial_z \phi = -\mathrm{i} \omega \zeta,\,z=0,\,\,\mathbf{x} \in \partial \Omega_{\mathrm{F}}, | ||
</math></center> | </math></center> | ||
<center><math> | <center><math> | ||
\mathrm{i} \omega \phi = -g\zeta,\,z=0,\,\,\mathbf{x} \in \partial \Omega_{\mathrm{F}}, | -\mathrm{i} \omega \phi = -g\zeta,\,z=0,\,\,\mathbf{x} \in \partial \Omega_{\mathrm{F}}, | ||
</math></center> | </math></center> | ||
where <math>\alpha = \omega^2/g </math>) | where <math>\alpha = \omega^2/g </math>) |
Revision as of 09:32, 28 April 2010
(note that the last expression can be obtained from combining the expressions:
where [math]\displaystyle{ \alpha = \omega^2/g }[/math])