dc.contributor.author |
Theocaris, PS |
en |
dc.date.accessioned |
2014-03-01T01:05:31Z |
|
dc.date.available |
2014-03-01T01:05:31Z |
|
dc.date.issued |
1974 |
en |
dc.identifier.issn |
0020-7403 |
en |
dc.identifier.uri |
https://dspace.lib.ntua.gr/xmlui/handle/123456789/8862 |
|
dc.subject.classification |
Engineering, Mechanical |
en |
dc.subject.classification |
Mechanics |
en |
dc.title |
Method of caustics for the study of cracked plates made of viscoelastic materials |
en |
heal.type |
journalArticle |
en |
heal.identifier.primary |
10.1016/0020-7403(74)90051-4 |
en |
heal.identifier.secondary |
http://dx.doi.org/10.1016/0020-7403(74)90051-4 |
en |
heal.language |
English |
en |
heal.publicationDate |
1974 |
en |
heal.abstract |
The optical method of caustics was used for the evaluation of the stress intensity factor at the crack tip in a viscoelastic plate made of polycarbonate of bisphenol A and containing a single external crack under conditions of generalized plane stress. It was assumed that the crack developed in a linear viscoelastic material. The reflected rays from both lateral faces, as well as the transmitted rays of a normally incident light beam were significantly dispersed at the close neighborhood of the crack tip because of the excessive lateral constraint and the strong variation of the refractive index, and concentrated along singular curves (caustics) at some distances from the plate. The reflected caustics formed two branches. While the internal branch, which was formed by reflections from the front face, depended only on the elastic modulus (E) and Poisson's ratio (v) of the material, the external branch, formed by reflections from the rear face, depended on E and v, as well as on the refractive index of the material (n). The transmitted rays formed the same type of caustic as that which was formed by reflections from the rear face, but with a different size. By studying the relative position and shape of the two reflected branches and their variation with time, information was derived concerning the viscoelastic state of the material at fracture. The transmitted light caustic was used as a check on the results. A series of viscoelastic tests in pure tension at various stress and strain levels yielded the variation of the mechanical (E, v) and optical (n, cr, cf) properties of the material with applied stress and strain. The values of these quantities at each stress level allowed the plotting of the relative positions of the two branches of the reflected caustics. Comparison of the actual position of the caustics at the crack tip with the caustic nomogram yielded the viscoelastic behavior of the material during the progress of loading. It was shown that by increasing the loading mode a strong viscoelastic behaviour was apparent which influenced considerably the fracture mode of the plate. © 1974. |
en |
heal.publisher |
PERGAMON-ELSEVIER SCIENCE LTD |
en |
heal.journalName |
International Journal of Mechanical Sciences |
en |
dc.identifier.doi |
10.1016/0020-7403(74)90051-4 |
en |
dc.identifier.isi |
ISI:A1974U786900001 |
en |
dc.identifier.volume |
16 |
en |
dc.identifier.issue |
12 |
en |
dc.identifier.spage |
855 |
en |
dc.identifier.epage |
860 |
en |