Conclusions
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1.
The second stage of creep in heat-resistant nickel alloys is due to changes in their intercrystalline structure.
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2.
With the same creep rate during the entire second period, which is characteristic of heat-resistant alloys containing a moderate amount of hardening phase equally distributed in the matrix, deformation is due to the gradual propagation of individual dislocations, leading to crystalline slip.
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3.
In alloys containing a substantial quantity of hardening phase creating a field of elastic distortion the deformation develops unevenly-the second state of creep has several sections with constant but differing rates of deformation. Each section is characterized by a different mechanism of the interaction of dislocation with growing particles of the hardening phase.
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4.
The low creep rate in the first section for alloy ÉI661 is due to pinning of dislocations around particles of γ′ phase; accelerated creep in the second section is due to the higher density of mobile dislocations; proparation of dislocations prevents particles of γ′ phase from growing together into platelets in the third stage with a lower creep rate.
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Literature cited
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Additional information
I. P. Bardin Central Scientific-Research Institute of Ferrous Metallurgy. Translated from Metallovedenie i Termicheskaya Obrabotka Metallov, No. 11, pp. 35–39, November, 1979.
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Travina, N.T., Nikitin, A.A. & Zimina, L.N. Dislocation arrays formed during creep of heat-resistant nickel alloys. Met Sci Heat Treat 21, 855–860 (1979). https://doi.org/10.1007/BF00708353
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DOI: https://doi.org/10.1007/BF00708353