Título: | STRENGTH OF PIPES WITH MACHINED DEFECTS | ||||||||||||
Autor: |
JORGE LUIZ COUTINHO DINIZ |
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Colaborador(es): |
JOSE LUIZ DE FRANCA FREIRE - Orientador RONALDO DOMINGUES VIEIRA - Coorientador |
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Catalogação: | 02/AGO/2002 | Língua(s): | PORTUGUESE - BRAZIL |
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Tipo: | TEXT | Subtipo: | THESIS | ||||||||||
Notas: |
[pt] Todos os dados constantes dos documentos são de inteira responsabilidade de seus autores. Os dados utilizados nas descrições dos documentos estão em conformidade com os sistemas da administração da PUC-Rio. [en] All data contained in the documents are the sole responsibility of the authors. The data used in the descriptions of the documents are in conformity with the systems of the administration of PUC-Rio. |
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Referência(s): |
[pt] https://www.maxwell.vrac.puc-rio.br/projetosEspeciais/ETDs/consultas/conteudo.php?strSecao=resultado&nrSeq=2813&idi=1 [en] https://www.maxwell.vrac.puc-rio.br/projetosEspeciais/ETDs/consultas/conteudo.php?strSecao=resultado&nrSeq=2813&idi=2 |
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DOI: | https://doi.org/10.17771/PUCRio.acad.2813 | ||||||||||||
Resumo: | |||||||||||||
According to Muhlbauer [1], 25% of the accidents with
pipelines are caused by corrosion. The aging of the
pipelines lead to an increase in the frequency accidents
associated with an increase in maintenance costs. To keep
accident frequency low, maintenance costs increase mainly
because the current methodologies to predict failure and
analyse pipe integrity are generally, overly conservatives.
The new inspection techniques coming forth and the
computers progress, it have justified the investment in
research and in the development of numeric methodologies to
preserve pipeline integrity and assure the economical
competitiveness of their operators. Nine tubular specimens
of steel API 5L X60, with 2 ms nominal length, 323 mms and
9.53 mms thickness were used. Defects were fabricated using
spark erosion to simulate corrosion. The defects had
residual thickness of 3 mm (30% of the nominal thickness),
95.3 mms width (10 times the nominal thickness) and lengths
between 250 and 525 mm. The pipe specimens were
instrumented with high elongation strain gage rosettes for
great plastic deformations and they were pressurized until
bursting. For the Finite element models were built based on
the geometries of the specimens. In this analysis it was
used the solid element of eight nodes because they demanded
a smaller processing time than the one of 20 nodes.
Regarding the shell element, the solid element of 8 nodes
represent better the defect`s geometry and gives the values
of elastoplastic strain along the thickness. Initially a
linear analysis was carried out. These analysis were
following by non-linear analysis, where it had been used
the real properties of the material in pipe. The values
obtained in these analysis were confronted with the
experimental values of the elastoplastic strain measured,
with the objective of validating the numeric model, had
being obtained good correlation. During the validation of
the model the numeric rupture criterion was analyzed to be
adopted. This analyses included an investigation on the
influence of small thickness variations , the influence of
the radius between walls of the defects, the optimum
increment of pressure and the importance of the mechanical
properties. This research does a complete analysis of the
tubular specimens, getting to develop a methodology able to
reproduce the experiment. All the factors that influence a
non-linear analysis were considered and the conclusion was
that the experimental rupture happens inside of a range of
values whose limits depend on the rupture criterion
adopted. It was verified that this range includes the
pressure that causes equivalent Misess stress equal to the
stress of materials in the first element and the numeric
instability. This instability happens when all of the
elements along the thickness, in any point of the defect,
reaches the equivalent Misess stress equal to the true
failure stress of the material. In the studied cases, this
range had distant limits amongst themselves of the order of
0.4 MPa, below 2% of the rupture pressure.
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