Template:Boundary value problem for a fixed body - Revision history

Meylan at 01:42, 21 August 2009

2009-08-21T01:42:05Z

@@ Line 1: / Line 1: @@
 The [[Standard Linear Wave Scattering Problem]]
 in [[Finite Depth]] for a fixed body is
-<center><math>
+{{standard linear wave scattering equations without body condition}}
-\nabla^{2}\phi=0, \, -h<z<0,\,\,\,\mathbf{x}\notin \Omega
+{{frequency domain equations for a rigid body}}

Meylan at 08:48, 24 August 2008

2008-08-24T08:48:02Z

← Older revision		Revision as of 08:48, 24 August 2008
Line 13:		Line 13:
	\frac{\partial\phi}{\partial n} = 0, \, \mathbf{x}\in\partial\Omega.		\frac{\partial\phi}{\partial n} = 0, \, \mathbf{x}\in\partial\Omega.
	</math></center>		</math></center>
	where <math>n</math> is the outward from the fluid) normal.		where <math>n</math> is the outward (from the fluid) normal.

Meylan at 08:47, 24 August 2008

2008-08-24T08:47:41Z

← Older revision		Revision as of 08:47, 24 August 2008
Line 11:		Line 11:
	</math></center>		</math></center>
	<center><math>		<center><math>
	\frac{\partial\phi}{\partial n} = 0, \, mathbf{x}\in\partial\Omega.		\frac{\partial\phi}{\partial n} = 0, \, \mathbf{x}\in\partial\Omega.
	</math></center>		</math></center>
	where <math>n</math> is the outward from the fluid) normal.		where <math>n</math> is the outward from the fluid) normal.

Meylan at 08:46, 24 August 2008

2008-08-24T08:46:41Z

← Older revision		Revision as of 08:46, 24 August 2008
Line 11:		Line 11:
	</math></center>		</math></center>
	<center><math>		<center><math>
	\frac{\partial\phi}{\partial z} = 0, \, z\in\partial\Omega.		\frac{\partial\phi}{\partial n} = 0, \, mathbf{x}\in\partial\Omega.
	</math></center>		</math></center>
			where <math>n</math> is the outward from the fluid) normal.

Meylan at 07:25, 24 August 2008

2008-08-24T07:25:57Z

New page

The [[Standard Linear Wave Scattering Problem]]
in [[Finite Depth]] for a fixed body is
<center><math>
\nabla^{2}\phi=0, \, -h<z<0,\,\,\,\mathbf{x}\notin \Omega
</math></center>
<center><math>
\frac{\partial\phi}{\partial z}=0, \, z=-h,
</math></center>
<center><math>
\frac{\partial\phi}{\partial z} = \alpha \phi,\,z=0,\,\,\mathbf{x}\notin\Omega,
</math></center>
<center><math>
\frac{\partial\phi}{\partial z} = 0, \, z\in\partial\Omega.
</math></center>