1995
DOI: 10.1007/bf02669429
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The transverse creep deformation and failure characteristics of SCS-6/Ti-6AI-4V metal matrix composites at 482 °C

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Cited by 11 publications
(3 citation statements)
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“…P is the Larson-Miller parameter, defined as P ¼ T(20 þ log t)10 À3 , where T is the absolute temperature and t the time in hours (in Figure 2, t is the time to failure). Data found in the literature for other composites and experimental conditions are also reported (Ohno et al, 1994;Eggleston and Ritter, 1995). This figure shows that the time to failure of the two SiC/Ti composites under investigation in this study is significantly greater than what is found in the literature.…”
Section: Transverse Creep Behavior -Macroscopic Scalesupporting
confidence: 72%
See 1 more Smart Citation
“…P is the Larson-Miller parameter, defined as P ¼ T(20 þ log t)10 À3 , where T is the absolute temperature and t the time in hours (in Figure 2, t is the time to failure). Data found in the literature for other composites and experimental conditions are also reported (Ohno et al, 1994;Eggleston and Ritter, 1995). This figure shows that the time to failure of the two SiC/Ti composites under investigation in this study is significantly greater than what is found in the literature.…”
Section: Transverse Creep Behavior -Macroscopic Scalesupporting
confidence: 72%
“…In fact, the environment may have a significant influence on the results. This assumption is confirmed by Eggleston and Ritter (1995) through SEM observations of an air tested specimen. They noted cracks in the gauge section of the surface corresponding to embrittlement of the titanium matrix by oxygen absorption.…”
Section: Transverse Creep Behavior -Macroscopic Scalesupporting
confidence: 60%
“…A number of scanning electron microscope (SEM) observations have shown that the only observed damage is interface debonding (Carrere, 2000). As shown in previous papers (Crossman et al, 1974;Ohno et al, 1994;Eggleston and Ritter, 1995), due to the existence of an experimentally determined critical stress ( c ), two distinct domains were evidenced as a function of the applied stress: below c , a slight damage (fibre/matrix debonding) is observed. After a short primary creep stage, a steady creep rate is attained leading to a long duration test without fracture, above this critical stress, damage is generalized, leading to an increase in the secondary creep rate and to the possible failure of the specimen.…”
Section: Introductionsupporting
confidence: 53%