dc.contributor.author |
Theocaris, PS |
en |
dc.date.accessioned |
2014-03-01T01:06:54Z |
|
dc.date.available |
2014-03-01T01:06:54Z |
|
dc.date.issued |
1987 |
en |
dc.identifier.issn |
00144851 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/9663 |
|
dc.subject |
Potential Function |
en |
dc.subject.other |
FRACTURE MECHANICS |
en |
dc.subject.other |
CRACK TIP |
en |
dc.subject.other |
INTERNAL OBLIQUE CRACKS |
en |
dc.subject.other |
PLANE STRESS CONDITIONS |
en |
dc.subject.other |
REFLECTED CAUSTICS METHOD |
en |
dc.subject.other |
SHEAR DISPLACEMENTS |
en |
dc.subject.other |
PLATES |
en |
dc.title |
KIII-Deformation modes in internal oblique cracks under plane-stress conditions |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1007/BF02319478 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1007/BF02319478 |
en |
heal.publicationDate |
1987 |
en |
heal.abstract |
The exact shape of the deformed internal oblique crack in an infinite elastic plate under conditions of plane stress was studied. The Muskhelishvili potential function yielded the exact stress and displacement field around the crack. While in previous papers by the author the study was mainly concerned with the definition of the in-plane shape of the deformed crack and important properties were disclosed concerning especially the contribution of the shear loading of the crack, in this paper the out-of-plane component of displacements is determined and its influence on the exact shape of the deformed crack in space is presented. It is shown that, as soon as shear displacements appear in the cracked plate under plane stress, out-of-plane shear displacements are a compulsory consequence for plane-stress conditions of the plate. The elliptic form of the deformed internal crack was twisted out of the plane of the plate with its zero twisting displacement near the new crack tip of its deformed shape corresponding to the vertex of the ellipse. The points of maximum and minimum out-of-plane displacements were placed close to the vertices of the ellipse at polar angles, θ, depending only on the eccentricity of the ellipse and displaced always on both sides of the vertices. The compulsory coexistence of mode II and mode III deformations makes the internal crack in plane stress to present a complicated pattern of deformation at its deformed crack tips. All of these results are amply supported by experimental evidence with caustics, which always show either a simple mode I pattern or a complex mode II and III pattern as soon as shear interferes in the mode of deformation of the plate. © 1987 Society for Experimental Mechanics, Inc. |
en |
heal.publisher |
Kluwer Academic Publishers |
en |
heal.journalName |
Experimental Mechanics |
en |
dc.identifier.doi |
10.1007/BF02319478 |
en |
dc.identifier.volume |
27 |
en |
dc.identifier.issue |
2 |
en |
dc.identifier.spage |
220 |
en |
dc.identifier.epage |
228 |
en |