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1.

Hurey I. 
Simulation model of dynamic processes during friction hardening of the flat surfaces [Електронний ресурс] / I. Hurey, V. Gurey, P. Dmyterko // Вісник Національного університету "Львівська політехніка". Оптимізація виробничих процесів і технічний контроль у машинобудуванні та приладобудуванні. - 2013. - № 772. - С. 80-85. - Режим доступу: http://nbuv.gov.ua/UJRN/VNULPO_2013_772_16
Розроблено імітаційну модель динамічних процесів під час фрикційного зміцнення плоских поверхонь деталей машин.
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2.

Gurey V. 
Machematical model of dynamic processes during friction hardening of flat surfaces [Електронний ресурс] / V. Gurey, V. Korendiy, P. Dmyterko // Вісник Національного університету "Львівська політехніка". Динаміка, міцність та проектування машин і приладів. - 2014. - № 788. - С. 79-85. - Режим доступу: http://nbuv.gov.ua/UJRN/VNULPDM_2014_788_15
Попередній перегляд:   Завантажити - 468.03 Kb    Зміст випуску     Цитування
3.

Dmyterko P. 
Research of Influence of Oscillations of Tool-Part System on Roughness of Surface Layer during High-Speed Friction Strengthening [Електронний ресурс] / P. Dmyterko, Y. Novitskyi, V. Gurey // Ukrainian journal of mechanical engineering and materials science. - 2016. - Vol. 2, Num. 1. - С. 47-54. - Режим доступу: http://nbuv.gov.ua/UJRN/ujmems_2016_2_1_7
During the discontinued friction strengthening except of the high-speed friction the processes of high-frequency shock loadings appears in the tool-part contact zone. The vibrations occur in the machine elastic system. During the vibrations of elastic systems, in the material of elastic elements and in the connecting units of the structure parts the energy dissipation into the ambient medium takes place. The energy dissipation of vibrations occurs due to the influence of the inelastic resistance forces on which the energy of the oscillatory system is spent. The vibrations of the tool-part system during the friction strengthening are similar to forced oscillations. However, for some particles of the part these oscillations are damped ones because the tool moves along the surface. The vibrations of the elastic system of the machine during the discontinued friction strengthening in the first approximation may be considered as free oscillations. For their investigation let us use the method of shock (impact) perturbation with a help of special measuring hammer which allows defining of the damping coefficient. With a help of the accelerometer and the hammer the shock (impact) curve and the registration curve of the tool-part vibrations were obtained. The obtained registration curve of tool-part vibrations was expanded into the Fourier series and with a help of MatLab program the obtained signal was filtered. Due to determination of the amplitude of vibrations and the oscillation period the logarithmic decrement of damping was defined. This parameter may be used for determination of the dynamic parameters of the oscillatory system of the converted machine. For defining the oscillations which arises in the part being machined we used the dynamometer, in which the piezo-crystal sensor was rigidly fixed. This sensor allows the readout of oscillations along three directions (along vertical, horizontal and transversal axis). Experimental research showed that the amplitude increased with increasing the number of processing modes and the oscillation character has exact wave-like form. The working process along the longitudinal direction has step-wise character. The single contact zone is heated to high temperatures; the metal softens; the friction coefficient decreases and the step-wise transportation of the part along the longitudal direction is being carried out. These phenomena are also confirmed by the figure of the machined surface and by the results of investigation of the topography of the machined surface. It is also experimentally determined that horizontal and vertical displacements of the spindle and the table vibrate with the frequencies close to resonance ones. With increasing of the tool rotation speed these vibrations have the character of damped ones and this phenomenon allows reducing the parameters of roughness, undulation and flatness of the surfaces being strengthened.
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4.

Zakharov V. 
Analysis and improvement of design diagrams and mathematical models of vibratory lapping machines [Електронний ресурс] / V. Zakharov, I. Kuzio, V. Korendiy, P. Dmyterko // Ukrainian journal of mechanical engineering and materials science. - 2019. - Vol. 5, Num. 3-4. - С. 44-56. - Режим доступу: http://nbuv.gov.ua/UJRN/ujmems_2019_5_3-4_9
Problem statement. The development of energy-efficient and high-performance vibratory lapping machines demands the improvement of their design diagrams and calculation techniques. Purpose. The main objectives of this research consist in detailed analysis of existent design diagrams and mathematical models of vibratory lapping machines; designing the three-mass hanger-type structures of such machines providing circular oscillations of laps; derivation of differential equations describing the motion of their oscillatory systems. Methodology. The technique of the research is based on fundamental concepts of engineering mechanics, strength of materials and theory of mechanical vibrations. Findings (results). The improved design diagrams of vibratory lapping machines with circular oscillations of laps are proposed and the corresponding differential equations describing the motion of the working elements are derived. Originality (novelty). The mathematical model of circular oscillations of the three-mass mechanical oscillatory system of vibratory lapping machine is developed. The possibilities of performing the double-side lapping of cylindrical and prismatic parts are considered. Practical value. The results of the performed investigations can be used during creating new designs and improving existent structures of vibratory finishing machines for lapping flat surfaces of cylindrical and prismatic parts. Scopes of further investigations. In further investigations, it is necessary to perform the numerical modelling of the system's motion using the derived differential equations, and to compare the obtained theoretical results with the results of experimental investigations.
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