For a stationary vertical plane, set U=0, sinθ=1, and cosθ=0. One integration of the steady equation, using h→h0 and vanishing derivatives far above the pool, gives
Put H=1+y and linearize to obtain y′′′=−3y. The two characteristic roots with positive real part are 31/3e±iπ/3. These are the modes that decay as X→−∞, so