Creep Rupture Due to Material Damage by Cavitation

Author:

Ragab A. R.1

Affiliation:

1. Department of Mechanical Design and Production, Faculty of Engineering, Cairo University, Giza, Egypt

Abstract

A phenomenological model to predict creep rupture times, based on material damage due to void growth and coalescence is presented. The model employs the Gurson-Tvergaard yield function together with the Norton-Baily power creep law. Rupture occurs at the end of a tertiary creep stage when the load-carrying capacity of the test-piece vanishes. Formulations for both uniaxial and triaxial conditions are given. Comparisons among the predictions of the present model and experiments for a vast number of data points indicate satisfactory agreement. A relation incorporating steady-state creep rate, rupture strain and rupture time is suggested. Furthermore acceptable correlation of the creep-rupture strength and creep strength to cause a specified creep strain is obtained.

Publisher

ASME International

Subject

Mechanical Engineering,Mechanics of Materials,Condensed Matter Physics,General Materials Science

Reference33 articles.

1. Hoff, N. J. , 1953, “Necking and Rupture of Rods under Tensile Loads,” ASME J. Appl. Mech., 20, p. 105105.

2. Kachanov, L. M. , 1958, “Time of the Fracture Process under Creep Conditions,” (in Russian) Izv. Akad. Nauk SSSR, No. 8, p. 2828.

3. Hancock, J. W. , 1976, “Creep Cavitation without a Vacancy Flux,” Metal Science, , 10, p. 319319.

4. Beere, W., and Speight, M. V., 1978, “Creep Cavitation by Vacancy Diffusion in Plastically Deforming Solid,” Metal Science, , 4, p. 172172.

5. Boyle, J. T., and Spence, J., 1983, Stress Analysis for Creep, Butterworths.

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