On the kinetic physical and mathematical metal creep theory controlled by thermally activated dislocation sliding

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详细

The rationale for the prospects of using the physical and mathematical theory of metal creep in creep computations is carried out by a comparative analysis of the classical phenomenological and physical and mathematical metal creep theories. On the example of the description by both theories specific results of non-stationary creep experiments and analysis of the theories equations it is shown that implementing the physical kinetic equation for the actual structural parameter of the material, namely the scalar density of immobile dislocations, makes the physical and mathematical theory universal for solving non-stationary metal creep problems with multiaxial loading, when change, including abruptly, temperature, forces and loading rates.

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作者简介

V. Greshnov

Ufa University of Science and Technology

编辑信件的主要联系方式.
Email: Greshnov_VM@list.ru
俄罗斯联邦, Ufa

R. Shaikhutdinov

Ufa University of Science and Technology

Email: shaykhutdinovri@gmail.com
俄罗斯联邦, Ufa

参考

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2. Fig. 1. Creep curve: I, the first unsteady stage; II, the second steady-state stage at which and has a minimum value; III, the third stage ending in the failure of the specimen. In the figure, where index c stands for creep characteristics and index e stands for elastic deformation characteristics.

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3. Fig. 2. Creep curve (εc in % of t in hours) of D16T alloy at temperature 150 °C and stress change from lower σ1 = 292 MPa (22 h) to higher σ2 = 340 MPa (14 h) (points - experiment [25], solid line - calculation according to physical and mathematical theory, dotted line - according to phenomenological theory of hardening).

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4. Fig. 3. Dependence of scalar density of fixed dislocations (ρs in cm-2 on t in hours) during creep of D16T alloy at temperature 150 °C and jumping change of stress from lower σ1 = 292 MPa (22 h) to higher σ2 = 340 MPa (14 h) (calculation by physical and mathematical theory of creep).

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5. Fig. 4. Creep curve (εc in % of t in hours) of D16T alloy at a temperature of 200 °C and a jumping change of stress from the higher σ1 = 160 MPa (24 h) to the lower σ2 = 120 MPa (26 h). Dots - experiment [25], solid curve - calculation (calculation according to the physical and mathematical theory of creep).

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