ATTRACTING MANIFOLDS FORMING FEATURES IN NEIGHBORHOOD OF CUTDOWN ENDMILLING TRAJECTORIES
Abstract and keywords
Abstract (English):
The work objective is to analyze the attracting manifolds generated under the endmilling. The formation of the periodic stationary trajectories of the tool deformation displacements in relation to the workpiece and their sustainability is previously considered. In this case, the movements form the attracting manifold defined by the trajectories of the periodic changes in the thickness and width of the cut-off layer by each cutter tooth taking into account the deformation displacements. As opposed to the previously considered cases, the paper focuses on the attracting manifolds generated at the buckling failure of the stationary trajectory. It is shown that depending on the system parameters and the process conditions in the dynamic milling system, the attracting manifolds of limit cycles, invariant tori, and strange (chaotic) attractors can be formed. In this context, two cases are analyzed. The first relates to the system parameters (primarily the cutting speed) which allow neglecting the coefficient variations in the differential equations within the impulsive reaction of the system. In the second case, the system parameters vary within the impulsive reaction of the system, and an additional source of the parametric self-excitation is formed in it. Considerable attention is paid to the analysis of the attracting manifold bifurcations in a parameter space: an overview and examples are provided. The attracting sets are analyzed from the perspective of their impact on the quality parameters of the parts production.

Keywords:
endmilling operation, attracting manifolds, bifurcations, control, quality parameters of parts production.
Text

В последние два десятилетия при изучении свойств эволюции и самоорганизации широко используется синергетическая парадигма [1–4]. Ее применение для управления сложными нелинейными объектами нашло свое отражение в работах [5–8]. При создании систем управления динамической системой резания также используются основы синергетической теории управления [7–14]. В этом случае управление, в том числе на основе построения программы ЧПУ, включает определение желаемых траекторий формообразующих движений и соответствующих им траекторий движения исполнительных элементов станка. При решении этой задачи принципиально важно знать свойства тех притягивающих множеств, которые самостоятельно образуются в окрестности формообразующих движений инструмента относительно обрабатываемой детали. Необходимо также уметь управлять этими множествами, влияющими на качество поверхности, формируемой при резании. Наконец, раскрытие свойств притягивающих множеств, формирующих сигнал виброакустической эмиссии, открывает новые пути построения информационных моделей для диагностирования процесса [15].

Изучение притягивающих множеств связано с рассмотрением динамической системы резания, изучению которой посвящено множество известных исследований [16–32]. Фрезерование является наиболее сложным процессом резания [33–46]. Это обусловлено его нестационарностью. Параметры длины и толщины срезаемого слоя каждым режущим лезвием периодически изменяются. Поэтому в подвижной системе координат, движение которой определяется траекториями исполнительных элементов, стационарным, установившимся состоянием является не точка равновесия (как при точении), а замкнутая траектория. В связи с этим уравнение динамики имеет периодически изменяющиеся коэффициенты.

Рассмотрим процесс фрезерования на станках, имеющих до пяти координат управления при обработке деталей, параметры жесткости которых существенно изменяются вдоль траектории движения инструмента [44–46]. В настоящей статье, в отличие от известных исследований, учитываются несколько источников самовозбуждения и связи, обусловленные взаимодействиями передней и задней поверхностей инструмента с деталью. Здесь можно рассматривать два случая. Первый — обработка с малыми частотами вращения шпинделя, когда в системе в пределах импульсной реакции параметры можно считать замороженными. Второй — обработка с большими частотами вращения, когда параметры нельзя считать замороженными.

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