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dc.contributor.advisorAmdahl, Jørgen
dc.contributor.advisorHeggelund, Svein Erling
dc.contributor.advisorStorhaug, Gaute
dc.contributor.authorJacobsen, Nanna Martine
dc.date.accessioned2015-10-05T15:05:23Z
dc.date.available2015-10-05T15:05:23Z
dc.date.created2015-06-09
dc.date.issued2015
dc.identifierntnudaim:13533
dc.identifier.urihttp://hdl.handle.net/11250/2350917
dc.description.abstractTorsion is highly important for large container carriers. In order to maximize the container capacity, a large deck area is essential, which often leads to a big bow are. To simplify loading and ooading, each cargo hold is equipped with huge hatch openings. These large deck openings, with slender longitudinal and transverse deck strips, will deform due to torsion in oblique seas, referred to as hatch opening distortions. This is regarded a vital strength aspect for container carriers. A master project is performed, in order to investigate how torsion contributes to extreme loading. Full scale measurements of a 8600 TEU container vessel, conducted by DNV GL, theoretical methods, and a global and a local Finite Element (FE) model have been used for this purpose. This was done, to get a greater knowledge of torsional behaviour of container carriers, which again can be used to document whether torsion should be included in ship design rules. The ship has been operating on two dierent trades. On Route 1, the vessel follows a relatively sheltered passage from Hamburg to Singapore, whereas the vessel crosses the North Pacic Ocean from Singapore to USA on Route 2. Results from a hydrodynamic analysis, and environmental data for each route, was used to calculate the long term distribution of longitudinal stresses in deck. Long term distribution of deck stresses veries that Route 2, which is known for more rough seas, gives the worst prediction of stresses. However, the measured stresses prove dierent. In order to nd out why measured stresses are higher for Route 1, although Route 2 has more rough seas, the vessel's operating speed was investigated. It was found that the vessel operates at higher speeds on Route 1, than on Route 2. With speed reduction, the ship resistance, and the risk for occurrence of high stresses due to wave induced vibrations, such as whipping, springing and torsional vibrations, is lowered. Additionally, no signicant routing has been observed on the rst route. On the second route, on the other hand, routing was found, i.e. the roughest seas have been avoided. This will again inuence and lower measured stresses. Speed reduction and routing are therefore important reasons why measured stresses are lower on Route 2, than Route 1, despite the fact that the wave environment is more rough on Route 2. Measurement data have been investigated to evaluate the degree of torsional vibrations present. During the day where most torsion is measured, the ratio of dynamic and wave stresses ~ 1.10, which indicates that the ship does not experience signicant torsional vibrations. Thus, torsional vibrations are found to be of minor concern for the 8600 TEU vessel. Global FE-analyses of the container vessel have been performed, with respect to the yielding criteria for Ultimate Limit State, ULS, due to torsion. Additionally, since many modications were done in order to analyse the model, self-checks of the model with vertical and horizontal bending moments were carried out. A coarse mesh was used to obtain nominal stresses. Rule stresses with respect to ULS were found by applying torsional moments, calculated from ship rules. The results show that maximum measured stresses in the deck strip are approximately 0.69-0.74 of ULS rule stresses for Route 1 and 0.63-0.68 on Route 2, i.e. measured stresses are within the acceptance criteria for ULS, on both routes. Since local stresses may be included in the measurements, the same analysis of the transverse deck strip was performed with ne mesh. Local stresses, and thus measured stresses, were found to be about 10 - 15 % higher than nominal stresses. The local stresses in the measurements are most likely due to the fact that the sensors are located close to hatch corners and close to a weld between two deck plates, which are source to stress concentrations, i.e. hot spot stresses. The magnitude of the hatch opening distortion has been calculated from the global FE-model. It was found that hatch opening distortion, due to the maximum measured stress of 131 MPa (measured on Route 1), has a magnitude of 226 mm. In comparison, the expected hatch opening distortion due to estimated ULS stresses is 335 mm at the deck strip where the sensors are located. The largest ULS hatch opening distortion obtained is located further forward, at cargo hold 3, where the deformations reaches 411 mm. The calculations were also done simplied, with use of hand calculations, 3D-Beam, and a deck strip model. This, to nd out if simplied and less time consuming methods can be used in later studies of hatch opening distortions, or if a global model must be used for this purpose. Values for hatch opening distortion for the simplied calculation methods are between 7 - 21 % lower than calculated from the global model. If further studies of other container ships gives the same relation between the simplied methods and the global model, simplied methods might be used, introducing a scaling factor.
dc.languageeng
dc.publisherNTNU
dc.subjectMarin teknikk, Marin konstruksjonsteknikk
dc.titleHull Monitoring and Assessment of Hatch Corners and Hatch Opening Distortion
dc.typeMaster thesis
dc.source.pagenumber141


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