Difference between revisions of "Template:Separation of variables for a dock"

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== Separation of Variables for a Dock ==
+
=== Separation of Variables for a Dock ===
  
The separation of variables equation for a dock
+
The separation of variables equation for a floating dock
 
<center>
 
<center>
 
<math>
 
<math>
\frac{\mathrm{d}^2 Z}{\mathrm{d} z^2} + k^2 Z =0.
+
Z^{\prime\prime} + k^2 Z =0,
 
</math>
 
</math>
 
</center>
 
</center>
Line 11: Line 11:
 
<center>
 
<center>
 
<math>
 
<math>
\frac{dZ}{dz}(-h) = 0
+
Z^{\prime} (-h) = 0,
 
</math>
 
</math>
 
</center>
 
</center>
Line 17: Line 17:
 
<center>
 
<center>
 
<math>
 
<math>
\frac{dZ}{dz}(0) = 0
+
Z^{\prime} (0) = 0.
 
</math>
 
</math>
 
</center>
 
</center>
 
The solution is  
 
The solution is  
<math>\kappa_{m}=m\pi/h</math>, <math>m\geq 0</math>. We define
+
<math>k=\kappa_{m}= \frac{m\pi}{h} \,</math>, <math>m\geq 0</math> and
 
<center>
 
<center>
 
<math>
 
<math>
\phi_{m}\left(  z\right)  =\frac{\cos k_{m}(z+h)}{\cos k_{m}h},\quad m\geq0
+
Z = \psi_{m}\left(  z\right)  = \cos\kappa_{m}(z+h),\quad
 +
m\geq 0.
 
</math>
 
</math>
 
</center>
 
</center>
as the vertical eigenfunction of the potential in the open
+
We note that
water region and
 
 
<center>
 
<center>
 
<math>
 
<math>
\psi_{m}\left(  z\right)  = \cos\kappa_{m}(z+h),\quad
+
\int\nolimits_{-h}^{0}\psi_{m}(z)\psi_{n}(z) \mathrm{d} z=C_{m}\delta_{mn},
m\geq 0
 
</math>
 
</center>
 
as the vertical eigenfunction of the potential in the dock
 
covered region. For later reference, we note that:
 
<center>
 
<math>
 
\int\nolimits_{-h}^{0}\phi_{m}(z)\phi_{n}(z) d z=A_{m}\delta_{mn}
 
</math>
 
</center>
 
where
 
<center>
 
<math>
 
A_{m}=\frac{1}{2}\left(  \frac{\cos k_{m}h\sin k_{m}h+k_{m}h}{k_{m}\cos
 
^{2}k_{m}h}\right)
 
</math>
 
</center>
 
and
 
<center>
 
<math>
 
\int\nolimits_{-h}^{0}\phi_{n}(z)\psi_{m}(z) d z=B_{mn}
 
 
</math>
 
</math>
 
</center>
 
</center>
 
where
 
where
<center><math>
 
B_{mn}=\frac{k_{n}\sin k_{n}h\cos\kappa_{m}h-\kappa_{m}\cos k_{n}h\sin
 
\kappa_{m}h}{\left(  \cos k_{n}h\right)  \left(  k_{n}
 
^{2}-\kappa_{m}^{2}\right)  }
 
</math></center>
 
and
 
 
<center>
 
<center>
 
<math>
 
<math>
\int\nolimits_{-h}^{0}\psi_{m}(z)\psi_{n}(z) d z=C_{m}\delta_{mn}
+
C_{m} =
 +
\begin{cases}
 +
h,\quad m=0 \\
 +
\frac{1}{2}h,\,\,\,m\neq 0
 +
\end{cases}
 
</math>
 
</math>
 
</center>
 
</center>
where
 
<center>
 
<math>
 
C_{m}=\frac{1}{2}h,\quad,m\neq 0 \quad \mathrm{and} \quad C_0 = h
 
</math></center>
 

Latest revision as of 23:20, 8 August 2009

Separation of Variables for a Dock

The separation of variables equation for a floating dock

[math]\displaystyle{ Z^{\prime\prime} + k^2 Z =0, }[/math]

subject to the boundary conditions

[math]\displaystyle{ Z^{\prime} (-h) = 0, }[/math]

and

[math]\displaystyle{ Z^{\prime} (0) = 0. }[/math]

The solution is [math]\displaystyle{ k=\kappa_{m}= \frac{m\pi}{h} \, }[/math], [math]\displaystyle{ m\geq 0 }[/math] and

[math]\displaystyle{ Z = \psi_{m}\left( z\right) = \cos\kappa_{m}(z+h),\quad m\geq 0. }[/math]

We note that

[math]\displaystyle{ \int\nolimits_{-h}^{0}\psi_{m}(z)\psi_{n}(z) \mathrm{d} z=C_{m}\delta_{mn}, }[/math]

where

[math]\displaystyle{ C_{m} = \begin{cases} h,\quad m=0 \\ \frac{1}{2}h,\,\,\,m\neq 0 \end{cases} }[/math]