Circular Basin: Difference between revisions

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<font color=red>'''UNDER  CONSTRUCTION'''</font>
<font color=red>'''UNDER  CONSTRUCTION'''</font>
=Analytical Solution=
=Analytical Solution=
Dupont (2001) presented an analytical solution for a closed circular domain on an f-plane, with radius , a linear bottom friction, and a spatially variable wind stress equal to , where is the gradient of the wind forcing and  is the vertical coordinate. The  water surface elevation solution is given by  
Dupont (2001) presented an analytical solution for a closed circular domain on an f-plane, with radius <math> R </math>, a linear bottom friction, and a spatially variable wind stress equal to <math> \tau_{Wx} = Wy/R</math>, <math> \tau_{Wy} = 0</math>
where <math> W</math> is the gradient of the wind forcing and <math> y</math> is the vertical coordinate. The  water surface elevation solution is given by  


{{Equation| <math> \eta =  
{{Equation| <math> \eta =  
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\frac{W{{f}_{c}}}{RgH\kappa }\left[ \frac{{{R}^{2}}}{8}+\frac{{{r}^{2}}}{4}\left( \frac{\kappa }{{{f}_{c}}}\sin 2\theta -1 \right) \right], & \mbox{if } f_c \ne0 \\
\frac{W{{f}_{c}}}{RgH\kappa }\left[ \frac{{{R}^{2}}}{8}+\frac{{{r}^{2}}}{4}\left( \frac{\kappa }{{{f}_{c}}}\sin 2\theta -1 \right) \right], & \mbox{if } f_c \ne0 \\
\end{cases}  </math> |2=1}}
\end{cases}  </math> |2=1}}
The current velocities are independent of the Coriolis parameter and are given by
{{Equation| <math> u = \frac{W y }{2R\kappa </math> |2=2}}
{{Equation| <math> v = -\frac{W x }{2R\kappa </math> |2=3}}


= Setup =
= Setup =

Revision as of 22:52, 11 May 2011

UNDER CONSTRUCTION

Analytical Solution

Dupont (2001) presented an analytical solution for a closed circular domain on an f-plane, with radius R, a linear bottom friction, and a spatially variable wind stress equal to τWx=Wy/R, τWy=0 where W is the gradient of the wind forcing and y is the vertical coordinate. The water surface elevation solution is given by

  η={Wr2sin2θ4gHR,if fc=0WfcRgHκ[R28+r24(κfcsin2θ1)],if fc0 (1)

The current velocities are independent of the Coriolis parameter and are given by

  Failed to parse (syntax error): {\displaystyle u = \frac{W y }{2R\kappa } (2)
  Failed to parse (syntax error): {\displaystyle v = -\frac{W x }{2R\kappa } (3)

Setup

The model is run to steady state from zero current and water level initial conditions with , , and both , and . Figure 1 shows the computational grid with 5 levels of refinement from 2000 m to 125 m.

Figure 1. Computational grid.



Results

Table 2. Goodness of fit statistics for the water elevation

Statistic Value
RMSE 0.0074 m
RMAE 0.0068
R^2 0.991
Bias 0.0017 m


References

  • Dupont, F., 2001. Comparison of numerical methods for modelling ocean circulation in basins with irregular coasts. Ph.D. thesis, McGill University, Montreal.



Test Cases

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