๐”– Bobbio Scriptorium
โœฆ   LIBER   โœฆ

Comparison between empirical and calculated stress intensity factors of hole edge cracks

โœ Scribed by J. Schijve

Publisher
Elsevier Science
Year
1985
Tongue
English
Weight
779 KB
Volume
22
Category
Article
ISSN
0013-7944

No coin nor oath required. For personal study only.

โœฆ Synopsis

Digitized data on crack growth of corner cracks at holes in a plate loaded in tension were published by Grandt and Macha. Empirical stress intensity factors were derived from these data. The empirical values were compared to stress intensity factors obtained by interpolation between calculated data of Raju and Newman. A satisfactory agreement was found.

NOTATIONS

crack length of through crack crack depth of quarter-elliptical crack crack length of quarter-elliptical crack correction factor for one corner crack instead of two symmetric comer cracks crack extension along curved crack front number of cycles shape factor hole radius plate thickness plate width polar angle 1000 psi = 6.90 MPa 1000 psi qin. = 1.099 MPa q/m I inch = 25.4 mm

๐Ÿ“œ SIMILAR VOLUMES

Stress intensity factors and interaction
Stress intensity factors and interaction of three cracks on both edges of finite width sheet
โœ H.M. Shu; J. Petit; Z.D. Jiang; G. Bezine ๐Ÿ“‚ Article ๐Ÿ“… 1993 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 698 KB

Ahatract-Two equal parallel cracks on one edge and one unequal parallel crack on the other edge of a Ii&e width sheet are studied. Formulae for calculating the stress intensity factors @IF) of this crack contiguration are obtained from the results of finite element analysis. The difference between t

Calculation of the stress intensity fact
Calculation of the stress intensity factor of an edge crack in a finite elastic disc using the weight function method
โœ G.A. Schneider; R. Danzer ๐Ÿ“‚ Article ๐Ÿ“… 1989 ๐Ÿ› Elsevier Science ๐ŸŒ English โš– 344 KB

A closed-form weight function formula is used to calculate the stress intensity factor of an edge crack in a finite elastic disc. The result is applied to the problems of a rotating disc and an infinite long cylinder under thermal shock.