Over het archief
In 2012 verloren we Jean Jacques Peters, voormalig ingenieur van het Waterbouwkundig Laboratorium (1964 tot 1979) en internationaal expert in sedimenttransport, rivierhydraulica en -morfologie. Als eerbetoon aan hem hebben we potamology (http://www.potamology.com/) gecreëerd, een virtueel gedenkarchief dat als doel heeft om zijn manier van denken en morfologische aanpak van rivierproblemen in de wereld in stand te houden en te verspreiden.
Het merendeel van z’n werk hebben we toegankelijk gemaakt via onderstaande zoekinterface.
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Modelling interactions between a ship's hull and a fluid mud layer Indekeu, B. (2016). Modelling interactions between a ship's hull and a fluid mud layer. MSc Thesis. KU Leuven. Faculteit Ingenieurswetenschappen: Leuven. xii, 119 pp.
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Thesis info:
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Beschikbaar in | Auteurs |
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Documenttype: Doctoraat/Thesis/Eindwerk |
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Abstract |
During the implementation of the model, the focus was on maximising flexibility. E.g. the rheologic parameters can easily be changed in the input of the model, as can the geometry of the object that is to be studied. Only one .stl file needs to be replaced and the forces on this new object are calculated automatically. The drag forces computed during the simulations of the different scenarios (combinations of a towing velocity and a draft) all fit within the interval set by the standard deviation of the experimental results. The computational effort required for the simulation of each of these scenarios differs. At higher velocities or very low drafts the computational effort will increase from 1h23, when the velocity equals 0.1m/s and the draft equals 10cm, over ±3h, when v = 0.3m/s and d = 6cm, to ±9h, when v = 0.5m/s and d = 2cm. This might seem like long simulation times for a two dimensional simulation, as the eventual goal is to simulate the flow around three dimsional objects. However these simulations were performed on a laptop with limited computational power and without the usage of parallel processing. The drag forces resulting from the simulation show to be very depended on the amount of structure (gamma) present, as on the aggregation coefficient a, the break-down coefficient b and their ratio bèta = b/a. When the initial condition of gamma increases, so will the drag force. The adjustment of a and b with a constant ratio bèta will primarily change the rate at which the stucture and therefore the drag force develops. The ratio bèta has a very important impact on the fluid behaviour. When bèta increases, the shear layer will widen and the maximal shear rate in this area will decrease. Finally, if modelling the interaction between a fluid mud and water layer is possible, CFD simulations could predict the forces acting on a ship’s hull. This would facilitate the determination the navigable depth (nautical bottom) for different shapes of hulls and for different maneuvers. |
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