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220 Fundamentals of Ocean Renewable Energy































            FIG. 8.16  Model domain decomposition for 10 processors. (Based on a model of the Alderney
            Race described in S.P. Neill, J.R. Jordan, S.J. Couch, Impact of tidal energy converter (TEC) arrays
            on the dynamics of headland sand banks, Renew. Energy 37 (1) (2012) 387–397.)



            However, due to load balancing, I/O, and overheads associated with commu-
            nication between parallel tasks, speedup for ocean models is nonlinear. For
            example, for the SWAN wave model applied to Galway Bay (Section 8.9.1),
            there is very little reduction in completion time once around 96 processors are
            exceeded. However, a job which uses >96 processors may take considerably
            longer to schedule, compared with a job which requests less resources.


            8.8 CFD MODELLING
            The dynamics of flow in both large (ocean tides/waves) and small scale (around
            a device) problems can be simulated by numerical solution of mass, momentum,
            and energy equations. Computational fluid dynamics (CFD) models (applied
            to small scales) and ocean models (applied to large-scale oceanic flows) are
            based on the Navier-Stokes equations. Further, CFD and ocean models use
            similar numerical techniques such as FDM or FVM. Although, strictly, ocean
            modelling is a subset of CFD, those working in the field of ocean energy make
            a clear distinction between what constitutes CFD, and what constitutes ocean
            modelling. CFD tends to be used for flows that are more isotropic (genuinely
            3D) than ocean applications, where the velocities in the horizontal direction are
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