Matches in SemOpenAlex for { <https://semopenalex.org/work/W199260214> ?p ?o ?g. }
Showing items 1 to 73 of
73
with 100 items per page.
- W199260214 abstract "Hyperbolic paraboloids have moved from being just an interesting mathematical form to being an extremely useful structural form. Early structural forms came into prominence in Europe in the middle 1930's when early versions were constructed out of concrete with little structural theory. After the Second World War, interest began to grow as a simple structural basis for the design of the hyperbolic structural form was documented. All early models were constructed in concrete using a simple shell theory. At the same time, academic research developed better understandings using small scale models. Following the initial excitement with the new form coupled with a growing understanding of the properties of reinforced concrete that fortuitously occurred at about the same time, interest then began to fade as other structural forms took over. Currently the last decade has seen a renewed interest in the form, but with a construction based on lattice members and not continuous shells. This interest has been driven by the desirability of a form to cover large areas without intermediate columns and the hyperbolic paraboloid fills this requirement. Formal research however has never progressed beyond small scale continuous shell or lattice models. This thesis aims to investigate the hyperbolic paraboloid using large scale shell and lattice structures. Models are created and examined in a range of three sizes up to 100 metres in plan dimensions. Of course, a model of such size cannot be constructed in the laboratory due to cost and size constraints and therefore this research is conducted using the finite element method and a computer program. This research covers bifurcation buckling and elastic geometric non-linear buckling of hyperbolic paraboloid continuous shells and lattices under changing rise to span ratio and changing edge beam flexural stiffness. Results from the shell models are compared with the results from the similar sized lattice models where possible. Steel lattice structures are also examined for their elastoplastic response. Firstly, geometrically perfect shell and lattice structures are examined for perfect load distribution and then asymmetric load distribution. It was found that in the case of the load variations, no significant effects eventuated. Secondly, shells and lattice structures are then examined to determine the influence that increasing levels of imposed imperfections have on their buckling behaviour and elastoplastic force distribution. These imperfections are introduced to simulate the fabrication and construction errors that occur in real structures. It was found that the introduction of these imperfections was generally not detrimental and sometimes even in severe levels actually increased buckling performance. The suggestion is made that this may be a way to create new structures based on a known structural model pedigree. Finally, the mathematical determination of hyperbolic paraboloid shell buckling pressure and buckling wavelength proposed in 1955 by Reissner was checked against the finite element results in these large scale shell models. It was found that the buckling pressure did not agree with the original Reissner formula and a modification to that formula is proposed by the author. Furthermore, it was found that the Reissner buckling wavelength did agree with finite element buckling results." @default.
- W199260214 created "2016-06-24" @default.
- W199260214 creator A5064237062 @default.
- W199260214 date "2012-02-01" @default.
- W199260214 modified "2023-09-26" @default.
- W199260214 title "A design and parametric study into large scale hyperbolic paraboloid shell and lattice structures" @default.
- W199260214 hasPublicationYear "2012" @default.
- W199260214 type Work @default.
- W199260214 sameAs 199260214 @default.
- W199260214 citedByCount "0" @default.
- W199260214 crossrefType "journal-article" @default.
- W199260214 hasAuthorship W199260214A5064237062 @default.
- W199260214 hasConcept C105795698 @default.
- W199260214 hasConcept C111472728 @default.
- W199260214 hasConcept C117251300 @default.
- W199260214 hasConcept C121332964 @default.
- W199260214 hasConcept C127413603 @default.
- W199260214 hasConcept C138885662 @default.
- W199260214 hasConcept C203231007 @default.
- W199260214 hasConcept C24890656 @default.
- W199260214 hasConcept C2524010 @default.
- W199260214 hasConcept C2776799497 @default.
- W199260214 hasConcept C2778755073 @default.
- W199260214 hasConcept C2780586882 @default.
- W199260214 hasConcept C2781052500 @default.
- W199260214 hasConcept C2781204021 @default.
- W199260214 hasConcept C33923547 @default.
- W199260214 hasConcept C62520636 @default.
- W199260214 hasConcept C78519656 @default.
- W199260214 hasConceptScore W199260214C105795698 @default.
- W199260214 hasConceptScore W199260214C111472728 @default.
- W199260214 hasConceptScore W199260214C117251300 @default.
- W199260214 hasConceptScore W199260214C121332964 @default.
- W199260214 hasConceptScore W199260214C127413603 @default.
- W199260214 hasConceptScore W199260214C138885662 @default.
- W199260214 hasConceptScore W199260214C203231007 @default.
- W199260214 hasConceptScore W199260214C24890656 @default.
- W199260214 hasConceptScore W199260214C2524010 @default.
- W199260214 hasConceptScore W199260214C2776799497 @default.
- W199260214 hasConceptScore W199260214C2778755073 @default.
- W199260214 hasConceptScore W199260214C2780586882 @default.
- W199260214 hasConceptScore W199260214C2781052500 @default.
- W199260214 hasConceptScore W199260214C2781204021 @default.
- W199260214 hasConceptScore W199260214C33923547 @default.
- W199260214 hasConceptScore W199260214C62520636 @default.
- W199260214 hasConceptScore W199260214C78519656 @default.
- W199260214 hasLocation W1992602141 @default.
- W199260214 hasOpenAccess W199260214 @default.
- W199260214 hasPrimaryLocation W1992602141 @default.
- W199260214 hasRelatedWork W1586422846 @default.
- W199260214 hasRelatedWork W195624662 @default.
- W199260214 hasRelatedWork W2010120793 @default.
- W199260214 hasRelatedWork W2023818102 @default.
- W199260214 hasRelatedWork W2042865060 @default.
- W199260214 hasRelatedWork W2045986532 @default.
- W199260214 hasRelatedWork W2059109770 @default.
- W199260214 hasRelatedWork W2059694388 @default.
- W199260214 hasRelatedWork W2093646939 @default.
- W199260214 hasRelatedWork W2101246713 @default.
- W199260214 hasRelatedWork W2264968833 @default.
- W199260214 hasRelatedWork W2292826546 @default.
- W199260214 hasRelatedWork W2326290315 @default.
- W199260214 hasRelatedWork W2794262639 @default.
- W199260214 hasRelatedWork W2914499912 @default.
- W199260214 hasRelatedWork W3185426257 @default.
- W199260214 hasRelatedWork W89315012 @default.
- W199260214 hasRelatedWork W952371700 @default.
- W199260214 hasRelatedWork W2135072027 @default.
- W199260214 hasRelatedWork W2186666578 @default.
- W199260214 isParatext "false" @default.
- W199260214 isRetracted "false" @default.
- W199260214 magId "199260214" @default.
- W199260214 workType "article" @default.