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When the force coefficients derived from experimental measurements were compared to the values predicted by CFD, the hexahedral mesh gave the most accurate predictions for the tug with no


fin. The average


discrepancy between the predicted side force component and the measured value was 6 percent and the maximum discrepancy was 13 per cent. The largest discrepancy between measured and predicted values occurred at 60 degrees of yaw. For the tetrahedral mesh the predicted forces are consistently under predicted by an average of 18 percent when compared to the measured values, with the maximum discrepancy being 24 per cent.


For the longitudinal force component, which was much smaller than the side force component at the operating yaw angles, the tetrahedral mesh had an average discrepancy of 1 percent and the hexahedral mesh had an average discrepancy of 4 percent.


Comparisons of the forces were made on the basis of the difference between the measured and predicted value of the force component non-dimensionalized by the total measured force ((Fx


2+Fy 4.2 HULL & FIN


Force components and non-dimensional coefficients derived from the results of the CFD simulations for the combined hull and fin are given for the tetrahedral and hexahedral meshes in Table 5. The results of the simulations are compared with the experiments in Figure 7.


2)0.5).


The experimental force data for the hull and fin condition was not available, since this was not a condition required for the original project. All of the experiments with a fin included the protective cage. The effect of the cage was estimated from the complete data set by subtracting the force components for the cage (estimated from the hull only condition and the hull and cage condition) from the hull, fin and cage condition.


The same observations about the accuracy of the


predicted forces apply to the tug with a fin as for the tug without the fin, but the differences between the results with different meshes are smaller. The hexahedral mesh resulted in predicted forces that were typically within 5 percent of the measured values, and never more than 10 percent different, whereas for the tetrahedral mesh, the typical agreement was within 7 percent and the maximum discrepancy was within 12 per cent. The force coefficients predicted from the hexahedral mesh were all within 5 percent of the experiment data for yaw angles between 30 and 40 degrees and within 10 percent at 45 degrees. The forces predicted by the tetrahedral mesh over this range were typically within 10 percent of the measured forces over the same range of yaw angle, but were consistently under


predicted relative to the


measured values. The force coefficients predicted by the hexahedral mesh were a good mean fit to the measured values up to 35 degrees of yaw, but above that the forces predicted by CFD are over predicted relative to the measured values.


Table 5, Comparison of CFD predictions of hydrodynamic forces, tug with fin  A


998.2 0.4849


Tetrahedral Mesh


Yaw angle, Speed, deg m/s 10 20 30 35 40 45


0.728 0.728 0.728 0.728 0.728 0.728


Hexahedral Mesh


Yaw angle, Speed, deg m/s 10 20 30 35 40 45


0.728 0.728 0.728 0.728 0.728 0.728


Surge, Total sway, N


N


7.712 6.173 3.721 2.065 0.523 -0.556


21.346 45.906 72.174 84.407 94.16


100.707


0.166 0.358 0.562 0.658 0.733 0.784


0.060 0.048 0.029 0.016 0.004 -0.004


89


102 115 119 128 145


Cq Cl # iterations


Surge, Total sway, N


N


5.878 3.752 1.22


0.418 -0.127 1.146


20.856 42.822 65.079 75.998 84.03 86.53


0.162 0.334 0.507 0.592 0.655 0.674


0.046 0.029 0.010 0.003 -0.001 0.009


224 259 284 293 310 428


Cq Cl # iterations


kg/m3 m2


©2008: Royal Institution of Naval Architects


B-47


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