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Título: NON-PROPAGATING CRACKS EXPERIMENTAL ANALYSIS
Autor(es): GUILHERME LIEBERENZ FALLEIROS MARIANTE
Colaborador(es): JAIME TUPIASSU PINHO DE CASTRO - Orientador
Catalogação: 12/NOV/2014 Língua(s): PORTUGUESE - BRAZIL
Tipo: TEXT Subtipo: SENIOR PROJECT
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.
Referência(s): [pt] https://www.maxwell.vrac.puc-rio.br/projetosEspeciais/TFCs/consultas/conteudo.php?strSecao=resultado&nrSeq=23674@1
[en] https://www.maxwell.vrac.puc-rio.br/projetosEspeciais/TFCs/consultas/conteudo.php?strSecao=resultado&nrSeq=23674@2
DOI: https://doi.org/10.17771/PUCRio.acad.23674
Resumo:
Fatigue damage is caused due to pulsing loads that, through sliding bands, create intrusions and extrusions on the material surface. Cracks iniciate on these micro damaged areas. Loads can act on the crack in mode I – traction, mode II – longitudinal shear stress, mode III – transverse shear stress, or in a combination of them. Crack iniciation is controlled by the stress range delta sigma , whereas its propagation is controlled by the stress intensity factor range deltaK. Cracks propagate whenever deltaK is bigger than the crack propagation threshold deltaKth. Short non-propagating cracks do not behave as the long ones. If the stress gradient around the cracks tip is large enough, the crack soon reaches a point where the stress around its tip is no longer big enough to propagate it, thus the crack stops.
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