Circular Basin: Difference between revisions

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= Setup =
= Setup =
[[Image:Grid_CB3.png|thumb|right|600px| Figure 1. Computational grid.]]
[[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 \text{m^2s^{-2}} </math>, <math> \kappa = 10^{-3} \text{s^{-1}} </math , and both <math> f_c = 0</math> and <math> f_c = 10^{-4} \text{s}^{-1} </math>. Figure 1 shows the computational grid with 5 levels of refinement from 2000 m to 125 m.
The model is run to steady state from zero current and water level initial conditions with <math> W = 10^-4 \text{m}^2 \text{s}^{-2} </math>, <math> \kappa = 10^{-3} \text{s}^{-1} </math , and both <math> f_c = 0</math> and <math> f_c = 10^{-4} \text{s}^{-1} </math>. Figure 1 shows the computational grid with 5 levels of refinement from 2000 m to 125 m.


'''Table 1. General Settings for Flow over a Bump'''
'''Table 1. General Settings for Flow over a Bump'''

Revision as of 23:00, 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 W=104m2s2, κ=103s1</math,andboth<math>fc=0 and fc=104s1. Figure 1 shows the computational grid with 5 levels of refinement from 2000 m to 125 m.

Table 1. General Settings for Flow over a Bump

Parameter Value
Time step 3600 s
Initial Water Depth 10 m
Linear Bottom Friction Coefficient 0.001



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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