具有两个非线性的双质量模型拖拉机振动的稳定性共振模式下的干摩擦类型

E. Kalinin, Y. Kolesnik, M. Myasushka
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Oscillations of the system with harmonic excitation by its base are considered (for example, the movement of a tractor on an uneven supporting surface). Oscillations of this system are described by nonlinear differential equations. To solve this equation, instead of friction dampers with friction forces, linear dampers with corresponding drag coefficients are included in the system. By solving the obtained system of linear inhomogeneous differential equations for the steady-state mode of oscillation, the amplitudes of oscillations of masses and deformation of springs with certain stiffness are determined. To clarify the effect of friction forces on mass oscillations in resonance modes, the obtained expressions were analyzed. A diagram of stability of mass oscillations in resonance modes is obtained. Conclusions. 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引用次数: 0

摘要

研究的目的是评估计算拖拉机振荡作为一个非线性系统的稳定性的可能性,如由于逆问题引起的干摩擦。研究方法。这项工作的方法论基础是对共振模式下双质量系统动力学的已知科学结果的概括和分析,以及系统方法的使用。运用分析法和比较分析法,形成科学问题,确定研究目标,制定研究目标。在建立实证模型时,运用了系统稳定性理论、系统分析方法和运筹学的主要规定。研究的结果。考虑系统在其基座的谐波激励下的振荡(例如,拖拉机在不平坦的支承表面上的运动)。该系统的振动用非线性微分方程来描述。为了求解该方程,在系统中加入具有相应阻力系数的线性阻尼器,而不是具有摩擦力的摩擦阻尼器。通过求解得到的稳态振动模式的线性非齐次微分方程组,确定了具有一定刚度的弹簧的质量振动幅值和变形幅值。为了阐明摩擦力对共振模式下质量振动的影响,对得到的表达式进行了分析。得到了共振模式下质量振荡的稳定性图。结论。已经确定,如果相对摩擦系数的值使其所确定的点位于1-2段和2-3段与坐标轴所围成的区域内,则在低频共振模式振荡过程中,摩擦力并不限制质量幅值波动的增加,而只是降低其增长速度。如果由相对摩擦系数确定的点位于1-1'-2'-3 '-3 -2-1区域,则弹簧具有间歇性变形,即在振荡期间,系统的一个质量相对于另一个质量停止,或最后一个质量相对于支撑面停止,或两个质量作为一个整体与支撑面一起移动周期的一部分。在高频共振时,如果相对摩擦系数的值使它们所确定的点不在4-5段和5-6段及坐标轴所包围的区域内,则摩擦力限制了质量振荡的幅度。第4-5节和第5-6节定义了共振时振动稳定性的边界(相对摩擦系数的临界比线)。
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STABILITY OF VIBRATIONS OF THE TRACTOR AS A TWO-MASS MODEL WITH TWO NONLINEARITIES OF THE TYPE OF DRY FRICTION IN RESONANCE MODES
Purpose of the study is to assess the possibility of calculating the stability of tractor oscillations as a system with nonlinearities such as dry friction due to the inverse problem. Research methods. The methodological basis of the work is the generalization and analysis of known scientific results regarding the dynamics of two-mass systems in resonance modes and the use of a systematic approach. The analytical method and comparative analysis were used to form a scientific problem, determine the goal and formulate the research objectives. When creating empirical models, the main provisions of the theory of stability of systems, methodology of system analysis and research of operations were used. The results of the study. Oscillations of the system with harmonic excitation by its base are considered (for example, the movement of a tractor on an uneven supporting surface). Oscillations of this system are described by nonlinear differential equations. To solve this equation, instead of friction dampers with friction forces, linear dampers with corresponding drag coefficients are included in the system. By solving the obtained system of linear inhomogeneous differential equations for the steady-state mode of oscillation, the amplitudes of oscillations of masses and deformation of springs with certain stiffness are determined. To clarify the effect of friction forces on mass oscillations in resonance modes, the obtained expressions were analyzed. A diagram of stability of mass oscillations in resonance modes is obtained. Conclusions. It has been established that if the coefficients of relative friction have such values that the point that is determined by them lies within the region bounded by segments 1-2 and 2-3 and coordinate axes, then during oscillations in the low-frequency resonance mode, the friction forces do not limit the increase in amplitudes fluctuations of masses, but only reduce the rate of their growth. If the point, which is determined by the coefficients of relative friction, lies in the region 1-1'-2'-3 '3-2-1, then the springs have intermittent deformation, that is, during the period of oscillation, one mass of the system has stops relative to another mass, or the last has stops relative to the support surface, or both masses move part of the period as a whole with the support surface. At resonance with a high frequency, the friction forces limit the amplitudes of mass oscillations if the coefficients of relative friction have such values that the point that is determined by them does not lie in the region bounded by segments 4-5 and 5-6 and the coordinate axes. Sections 4-5 and 5-6 define the boundaries of vibration stability at resonance (lines of critical ratios of the coefficients of relative friction).
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