A rectangular sheet containing a central crack subjected to a normally incident anti-plane shear wave, is discussed in this paper. With the aid of the basic theorem of the Fourier transform and Fourier series, the solution of the dynamic stress intensity factor of this problem may be given by means
A rectangular sheet with an edge crack excited by a normal anti-plane shear wave
โ Scribed by X.S. Zhang
- Publisher
- Elsevier Science
- Year
- 1989
- Tongue
- English
- Weight
- 360 KB
- Volume
- 34
- Category
- Article
- ISSN
- 0013-7944
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โฆ Synopsis
Making use of the basic theorem of the Fourier cosine transform and Fourier sine series, the solution of the dynamic stress intensity factor of a rectangular sheet containing an edge crack subjected to a normally incident anti-plane shear wave, is found in the study. We can easily verify that the problems of a strip and a half plane with an edge crack excited by a normally incident anti-plane shear wave, are the special cases of the solution in this article. Especially, it is of interest to note that all of the solutions to the dynamic stress intensity factor of the subject are identical with those results in the work by S. W.
๐ SIMILAR VOLUMES
With the aid of the basic theorem of the Fourier cosine transform and Fourier sine series, the general solution of the dynamic stress intensity factor of a finite rectangular plate containing a pair of edge cracks excited by a normal anti-plane shear wave is found in the present paper. We can easily
## Abstrsel-Application of the basic theorem of the Fourier cosine transform and Fourier sine series to this study, we can find the general solution of an eccentric crack normal to two interfaces among three layers in a finite rectangular sheet loaded by an arbitrary longitudinal shear stress. It
Fourier ~~sfo~ and Fourier series technique is used to express the stress intensity factor of a centra1 crack in P finite rectangular sheet with two different materials whose interface normat to the crack in terms of the solution of a Fredhogm integral equation of the second kind. The constant loadi