“…These curves were constrained by the values of R P ,1 ( λ = 5) = 0.001, R P ,2 ( λ = 5) = 0.01, R P ,4 ( λ = 5) = 0.5, and R P ,1–4 ( λ = 0) = 0. The scenario R P ,4 ( λ ) reflected the upper boundary value for the damping factor equal to R P ,3 ( λ = 24) from the observations in Morén et al (), while R P ,1 ( λ ) and R P ,2 ( λ ) reflected values of R p at λ = 5 m one and two orders of magnitude lower than the observations. Furthermore, from the theory of open channel flow during steady flow conditions, d D WS /d Z BS = (d D WS /d x )/(d Z BS /d x ) = 1/( Fr 2 –1), which implies decreasing water surface ( D WS ) fluctuations in comparison to bed surface ( Z BS ) fluctuations with decreasing Froude number.…”