Article ID | Journal | Published Year | Pages | File Type |
---|---|---|---|---|
1574004 | Materials Science and Engineering: A | 2015 | 11 Pages |
Abstract
Creep deformation and rupture behaviour of 9Cr-1.8W-0.5Mo-VNb steel have been investigated at 873Â K, 923Â K and 973Â K over a stress range of 80-220Â MPa. The absence of clear primary creep regime and prolonged secondary stage of creep deformation have been noticed under lower stress level at 973Â K. The variation of minimum creep rate with applied stress obeyed Norton's power law of creep. The apparent stress exponents of 15.2, 12.3 and 5.8, and apparent activation energy of 619Â kJ/mole have been estimated for creep deformation of the steel. The apparent stress exponents and activation energy have been rationalised on the basis of threshold stress. The threshold stress values of 137.5Â MPa, 83.3Â MPa and 29.7Â MPa were obtained at 873Â K, 923Â K and 973Â K respectively. The threshold stress compensated true stress exponent of 4 and true activation energy of 244Â kJ/mole, and threshold stress normalised by Orowan stress confirms that the lattice diffusion assisted localised climb of dislocation is the rate controlling of creep deformation in the steel. The steel obeyed Monkman and modified Monkman-Grant relationships. Damage tolerance factor of 6 in the steel demonstrates that the microstructural degradation such as coarsening of precipitates and subgrain structure is the dominant creep damaging mechanism in the steel.
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Physical Sciences and Engineering
Materials Science
Materials Science (General)
Authors
T. Sakthivel, S. Panneer Selvi, K. Laha,