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

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The equations
 
The equations
of motion in the time domain, in non-dimensional
+
of motion in the time domain are
form, so that gravity is unity, are
 
 
Laplace's equation through out the fluid
 
Laplace's equation through out the fluid
 
<center><math>
 
<center><math>
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surface we have the kinematic condition
 
surface we have the kinematic condition
 
<center><math>
 
<center><math>
\partial_{t}\zeta=\partial_{n}\Phi,\ \ z=0,\ x\in F,
+
\partial_{t}\zeta=\partial_{n}\Phi,\ \ z=0,\ x\in \partial\Omega_{F},
 
</math></center>
 
</math></center>
 
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.
+
\partial_{t}\Phi = -g\zeta ,\ \ z=0,\ x\in \partial\Omega_{F}.
 
</math></center>
 
</math></center>

Latest revision as of 23:14, 22 April 2010

The equations of motion in the time domain 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 \partial\Omega_{F}, }[/math]

and the dynamic condition (the linearized Bernoulli equation)

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