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Reflection coefficient for different wave damping method and different waves 

Reflection coefficient for different wave damping method and different waves 

Source publication
Conference Paper
Full-text available
Simulating free-surface flow around ships in sea waves using RANSE-Methods usually requires damping of the waves in front of the outlet to avoid reflections. It has been shown, that common damping methods like sponge layer methods deliver a reliable damping for monochromatic waves, but require a parameter adjustment by the user for different wave s...

Context in source publication

Context 1
... scale factor χ is varied from 0.008 to 1.0 for each wave to achieve the least reflections and to show the dependency of our wave damping method from the wave characteristics. Figure 2 shows the results of all simulations. Sub- figure b shows the results of the common linear sponge layer method (with f 2 = 0.0 = const), also implemented in our solver. ...

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Citations

... In Söding's paper, the need for an explicit added mass matrix for numerical stability is explained, and an iteration-based method for its determination is formulated. In a study by Meyer et al. [25], this algorithm was applied to calculate the motion of a yacht in head waves. To the best of our knowledge, no thorough demonstration of the stability properties exists in the literature, and no open-source CFD implementation is available to the scientific community. ...
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... In Söding's paper, the need for an explicit added mass matrix for numerical stability is explained and an iteration based method for its determination is formulated. In a study by Meyer et al. [25] this algorithm was applied to calculate the motion of a yacht in head waves. To the best of our knowledge, no thorough demonstration of the stability properties exists in the literature, and no open source CFD implementation is available to the scientific community. ...
... The pressure parts of the hydrodynamic force and torque contain components, that are proportional to the instantaneous body acceleration, and which go into the total force-torque vector, f , in Eqn. (25). Just as we did in the introductory 1-DoF example, we can conceptually split f into a part, −Av b , containing all terms that are proportional tov b , and another part, f other , containing all other forces and torques, ...
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