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INTRODUCTIONThe structural evolution of metallic materials dur ing plastic deformation has been extensively studied for the last hundred years. As a result, the most impor tant sign of a plastic flow was found to be the localiza tion of plastic deformation, which is accompanied by the localization and intensification of heat sources in a material. When calculating the intensity of heat sources in a material and determining the total energy consumed for its deformation, one can perform an integral estimation of the energy stored in an ensemble of mesodefects in order to determine the current stage of its evolution.The thermodynamic and mechanical features of the elastic-plastic transition were studied in [1][2][3][4][5][6][7]. In [1], we proposed a method to estimate the energy stor age rate in a material using the results of infrared scan ning. In [2], this process was considered from the for mal points of the mechanics of continua using an additionally introduced structure sensitive tensor variable, which describes the growth of mesoscopic defects. The wave character of heat dissipation in steel during the elastic-plastic transition was first experi mentally detected in [3]. The authors of [4] experi mentally studied the propagation of deformation localization waves in fcc metal single crystals (copper, nickel). Then, researchers used speckle interferometry and detected wave deformation processes in a wide range of plastic and quasi plastic materials. Kiselev [5] suggested a mathematical model for the propagation of localized plasticity waves in crystals; it is based on the double cross slip of screw dislocation segments.In this work, we continue the study of the energy dissipation [1, 2] during the elastic-plastic transition by infrared scanning. We determine the main thermo physical features of this transition at various strain rates and study the temperature kinetics of the sample and the dependence of the heat wave velocity on the number of waves and the strain rate.
EXPERIMENTALWe investigated the elastic-plastic transition in iron subjected to uniaxial quasi static tension. The chemical composition of iron is given in the table.The experiment was carried out under isothermal conditions. The strain rate was varied from 10 -4 to 2 × 10 -3 s -1. To obtain reliable results, we analyzed two series of samples that were made from the same batch of armco iron and subjected to the same mechanical and heat treatment.After mechanical treatment, the samples were annealed in an oxygen free atmosphere at 800°C for 8 h. The oxygen free atmosphere was created by simulta neous annealing of the iron samples under study and additional copper samples with a developed surface.The geometry of the iron samples is shown in Fig. 1 Abstract-The structural and thermo...