Difference between revisions of "Template:Equations of motion time domain without body condition"

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Laplace's equation through out the fluid
 
Laplace's equation through out the fluid
 
<center><math>
 
<center><math>
\Delta\Phi\left(  \mathbf{x,}t\right)  =0,\ \ \mathbf{x}\in\Omega,
+
\Delta\Phi\left(  \mathbf{x,}t\right)  =0,\ \ \mathbf{x}\in\Omega.
 
</math></center>
 
</math></center>
 
At the bottom surface we have no flow
 
At the bottom surface we have no flow
Line 17: Line 17:
 
and the dynamic condition (the linearized Bernoulli equation)
 
and the dynamic condition (the linearized Bernoulli equation)
 
<center><math>
 
<center><math>
\zeta = -\partial_{t}\Phi,\ \ z=0,\ x\in F,
+
\zeta = -\partial_{t}\Phi,\ \ z=0,\ x\in F.
 
</math></center>
 
</math></center>

Revision as of 11:31, 21 August 2009

The equations of motion in the time domain, in non-dimensional form, so that gravity is unity, are Laplace's equation through out the fluid

[math]\displaystyle{ \Delta\Phi\left( \mathbf{x,}t\right) =0,\ \ \mathbf{x}\in\Omega. }[/math]

At the bottom surface we have no flow

[math]\displaystyle{ \partial_{n}\Phi=0,\ \ z=-h. }[/math]

At the free surface we have the kinematic condition

[math]\displaystyle{ \partial_{t}\zeta=\partial_{n}\Phi,\ \ z=0,\ x\in F, }[/math]

and the dynamic condition (the linearized Bernoulli equation)

[math]\displaystyle{ \zeta = -\partial_{t}\Phi,\ \ z=0,\ x\in F. }[/math]