G0/ . Since the value of the ledge force can be neglected as compared with the other two forces in (I), we get ~c = [ b / ~( 1 -v 2 ) ] ~2 / K I 2 ( 2 )
Response: Discussion of “Prediction of threshold stress intensity for fatigue crack growth using a dislocation model,” by A. T. Yokobori, Jr.
✍ Scribed by K. Sadananda; P. Shahinian
- Publisher
- Springer Netherlands
- Year
- 1978
- Tongue
- English
- Weight
- 169 KB
- Volume
- 14
- Category
- Article
- ISSN
- 1573-2673
No coin nor oath required. For personal study only.
✦ Synopsis
We express our appreciation to Dr. Yokobori for his interest in our paper [l] and for bringing to our attention their earlier paper [2] on dislocation dynamics theory for fatigue crack growth. The discussion of our paper centers on two points, namely that the dislocation models in [I] and [2] are essentially the same, except [2] was published earlier, and a more important issue that there should be two requirements to be satisfied before a dislocation can be nucleated at the crack tip. These requirements are the stress and energy which are claimed to providerespectively -the necessary and sufficient conditions for the dislocation generation.
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