NON-PROPAGATION CONDITIONS (DELTA-K(TH)) AND FATIGUE-CRACK PROPAGATION THRESHOLD (DELTA-K(T))

Authors
Citation
G. Marci, NON-PROPAGATION CONDITIONS (DELTA-K(TH)) AND FATIGUE-CRACK PROPAGATION THRESHOLD (DELTA-K(T)), Fatigue & fracture of engineering materials & structures, 17(8), 1994, pp. 891-907
Citations number
32
Categorie Soggetti
Material Science","Engineering, Mechanical
ISSN journal
8756758X
Volume
17
Issue
8
Year of publication
1994
Pages
891 - 907
Database
ISI
SICI code
8756-758X(1994)17:8<891:NC(AFP>2.0.ZU;2-J
Abstract
Fatigue crack propagation threshold values have been determined with t wo experimental methods, i.e., the constant R method and the constant K(max) method. Three materials, namely Al7075-T7351 and Ti6Al4V STA in the LT- and TL-orientations, and a Ti-turbine disk material (IMI 685) in the CR-orientation, were investigated. The paper is divided into 3 parts. In the first part the test conditions, the experimental result s and the conclusions drawn from the experimental results are presente d, namely that the three different functional dependencies of DELTAK(t h) on R cannot be reconciled with present continuum mechanics concepts . In the second part, some facts used in conjunction with the da/dN - DELTAK(eff) methodology are applied to the non-propagation condition D ELTAK(th). Parameters such as K(op), the threshold DELTAK(T), and a pa rameter ''K(LL)'' are investigated by numerical modelling of their ind ividual influence on the DELTAK(th) versus R curves. This modelling wo rk shows that the individual DELTAK(th) versus R curves are primarily dependent on the K(op) behavior of the respective material. Further, i t is shown that the threshold DELTAK(T) is a constant value, independe nt of any particular cyclic loading condition. In the third part of th e paper, the DELTAK(eff) concept is applied to the experimental result s obtained in the first part. Using either experimentally or semi-empi rically determined K(op) functions and the measured DELTAK(T) values, the DELTAK(th) versus R curves of the three materials investigated wer e accurately reconstructed. It follows that the DELTAK(th) versus R cu rves of the individual materials are the natural consequence of the dr iving force for fatigue crack propagation, namely DELTAK(eff).