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210 Fundamentals of Ocean Renewable Energy


            8.3.1 Turbulence Closure
            For large Reynolds numbers (>2000), the flow velocity experiences fluctuations
            around the mean velocity. Common numerical models cannot simulate these
            fluctuations, because they occur over very small timescales (e.g. fractions
            of seconds). Alternatively, they replace the velocity by mean and fluctuating
            components as follows

                                        u = u +´u                      (8.29)
            where u is the time averaged and ´u is the fluctuating part. Tidal models simulate
            the temporal average rather than the actual velocity (u) to avoid this issue. The
            argument is that these small and rapid fluctuations in velocity are not important,
            compared with the mean velocity that is of relevance to tidal energy generation.
            The time average of the fluctuating velocity is zero. Therefore, if the Navier-
            Stokes equations were linear, we could just replace velocities by time averaged
            velocities. To make this point clearer, consider the continuity equation, which is
            a linear equation. Taking a moving time average leads to

                                            ∂u   ∂v  ∂w
                                              +    +      dt = 0       (8.30)
                                         T  ∂x   ∂y   ∂z
                             ∂(u +´u)  ∂(v +´v)  ∂(w +´w)

                                    +         +           dt = 0       (8.31)
                               ∂x        ∂y        ∂z
                          T
            Also, for the x component of velocity (and similarly for the other components),
            we have

                            ∂u    ∂  T  udt  ∂  T  ´ udt  ∂  T  udt

                              dt =       +         =        + 0        (8.32)
                          T ∂x       ∂x       ∂x       ∂x
            Because the average of the fluctuating velocity is zero, the time averaged
            continuity equation simply becomes
                                    ∂u   ∂v   ∂w
                                       +   +     = 0                   (8.33)
                                    ∂x   ∂y   ∂z
            Unfortunately, this is not the case for the nonlinear parts of the momentum
            equation. For instance, if we just consider the convective acceleration term in
            the momentum equation, (see Chapter 2) we have
                              ∂u               ∂(u +´u)

                             u   dt =    (u +´u)        dt             (8.34)
                            T ∂x      T          ∂x
                                        ∂u         ∂ ´u

                                   =   u   dt +  ´ u  dt + 0 + 0       (8.35)
                                      T ∂x      T ∂x
                                        ∂u        1 ∂ ´u
                                                     2
                                   =   u   dt +       dt               (8.36)
                                      T ∂x      T 2 ∂x
                                     2
            Because the time average of ´u is not zero (in contrast to ´u), additional terms
            appear in the momentum equation. For instance, the convective acceleration
            term after time averaging becomes
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