dc.contributor.author |
Theocaris, PS |
en |
dc.contributor.author |
Petrou, L |
en |
dc.date.accessioned |
2014-03-01T01:06:56Z |
|
dc.date.available |
2014-03-01T01:06:56Z |
|
dc.date.issued |
1987 |
en |
dc.identifier.issn |
03769429 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/9687 |
|
dc.subject |
Closed Form Solution |
en |
dc.subject |
Exact Solution |
en |
dc.subject |
Potential Function |
en |
dc.subject |
Singular Solution |
en |
dc.subject |
Stress Intensity Factor |
en |
dc.subject.other |
MATHEMATICAL TECHNIQUES - Curve Fitting |
en |
dc.subject.other |
STRESSES - Evaluation |
en |
dc.subject.other |
CAUSTIC GENERATRIX CURVE |
en |
dc.subject.other |
CRACK-TIP SINGULARITY |
en |
dc.subject.other |
INFINITE PLATE |
en |
dc.subject.other |
STRESS INTENSITY FACTOR |
en |
dc.subject.other |
PLATES |
en |
dc.title |
On the equivalent order of crack-tip singularity defined by caustics |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1007/BF00276357 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1007/BF00276357 |
en |
heal.publicationDate |
1987 |
en |
heal.abstract |
The problem of a transverse Griffith crack in an infinite plate submitted to simple tension at infinity was studied by using its closed form solution described by the elastic potential function φ{symbol}(z). The exact form of the caustic and its generatrix curve formed around the crack tips was exactly described by using the φ{symbol}(z)-function. These exact forms were compared with the respective forms given either by the singular one-term solution of the problem and accepting that the order of singularity at the crack tip is (1/2), or by a solution defining the order of singularity and the respective stress intensity factor by taking into consideration the influence of the distance from the crack tip where these quantities are evaluated. It was shown by comparing the first stress invariant I1, whose gradient defines the respective caustic, that the differences between the exact values and the values of I1 derived by the proposed method with variable order of singularity is much smaller than the differences between the exact solution and the singular solution. The singular solution is based on the assumption of a constant value of the order of singularity. © 1987 Martinus Nijhoff Publishers. |
en |
heal.publisher |
Kluwer Academic Publishers |
en |
heal.journalName |
International Journal of Fracture |
en |
dc.identifier.doi |
10.1007/BF00276357 |
en |
dc.identifier.volume |
35 |
en |
dc.identifier.issue |
4 |
en |
dc.identifier.spage |
269 |
en |
dc.identifier.epage |
282 |
en |