For an irrotational flow, write . The incompressible flow condition then gives the Laplace equation
At leading order in a small disturbance this equation holds on . Including gravity, the Unsteady Bernoulli equation is
Choose the time-dependent additive freedom in the velocity potential so that . Neglecting surface tension, pressure continuity at the free surface gives the exact dynamic condition
The free surface is a material boundary: applying the material derivative to yields the kinematic boundary condition for a free-surface graph
For a small disturbance, the Taylor expansion from to changes the first-order velocity potential and its partial derivatives only at second order. Both and are also second-order terms. The linearized free-surface boundary conditions are therefore
The fixed bed has the no-penetration boundary condition
The required approximation is small surface elevation, small wave steepness, and small velocity perturbations. The stated alone does not ensure this approximation near resonance.

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