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Investigation of the creep and micropolar creep of various materials under static and dynamic loads

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Abstract

Creep is investigated under a uniform stress state with allowance for the micropolar creep of the following materials: lignostone (T=293°K), steel ON2M (T=773° K), and an AIMgSi aluminum alloy (T= 293° K) understate and cyclic tension, i.e., atA σ = σam = 0, 0.25, and 0.5. It is established that for lignostone, the microstrains I11 are two orders lower than 2ε12 in torsion, and the values of 2l12 are only a half order lower than ε11 in tension. The creep strain of lignostone is described using nonlinear theory of viscoelasticity. For alloys and metals under static creep, the value of Iij is two or three orders lower than εij A qualitative change in microipolar creep occurs in the case of dynamic loading: whenA σ = 0.5,the ratio of values of fatigue creep rate 211212 = 0.2.

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Literature cited

  1. A. K. Eringen, Theory of Micropolar Creep [Russian translation], Vol. 2: Failure, Mir, Moscow (1975).

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  2. M. Czech, “Nonlinear anisotropic model of the creep description of lignostone,” Fourth International Symposium on Creep and Coupled Processes, Bialystok (1992).

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A subject investigated in 1990 with funding provided by the Ministry of National Education.

Translated from Problemy Prochnosti, No. 12, pp. 18–23, December, 1993.

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Yakovlyuk, A., Czech, M., Pleva, M. et al. Investigation of the creep and micropolar creep of various materials under static and dynamic loads. Strength Mater 25, 870–874 (1993). https://doi.org/10.1007/BF00774632

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  • DOI: https://doi.org/10.1007/BF00774632

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