نبذة مختصرة : The potential flow equations which govern the free–surface motion of an ideal fluid (the water wave problem) are notoriously difficult to solve for a number of reasons. First, they are a classical free– boundary problem where the domain shape is one of the unknowns to be found. Additionally, they are strongly nonlinear (with derivatives appearing in the nonlinearity) without a natural dissipation mechanism so that spurious high–frequency modes are not damped. In this contribution we address the latter of these difficulties using a surface formulation (which addresses the former complication) supplemented with physically–motivated viscous effects recently derived by Dias, Dyachenko, and Zakharov (2008). The novelty of our approach is to derive a weakly nonlinear model from the surface formulation of Zakharov (1968) and Craig & Sulem (1993), complemented with the viscous effects mentioned above. Our new model is simple to implement while being both faithful to the physics of the problem and extremely stable numerically.
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