Circular Basin: Difference between revisions

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= Setup =
= 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.
[[Image:Grid_CB3.png|thumb|right|600px| Figure 1. Computational grid.]]
The model is run to steady state from zero current and water level initial conditions with <math> W = 10^-4 m^2s^{-2},  , and both , and . Figure 1 shows the computational grid with 5 levels of refinement from 2000 m to 125 m.


[[Image:Grid_CB3.png|thumb|right|600px| Figure 1. Computational grid.]]


   
   

Revision as of 22:55, 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

  u=Wy2Rκ (2)
  v=Wx2Rκ (3)

Setup

Figure 1. Computational grid.

The model is run to steady state from zero current and water level initial conditions with <math> W = 10^-4 m^2s^{-2}, , and both , and . Figure 1 shows the computational grid with 5 levels of refinement from 2000 m to 125 m.



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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