In the present work, we consider the optimization of a two-flow, three-stage modular gear by means of a redesigned mechanical drive for beam pumps. Oscillations of modular-gear shafts with added gears and two-crown gear modules arise under the action of external periodic forces at the point of beam suspension and are related to elastic deformation of the mechanical system. Small oscillations relative to the equilibrium position become dangerous for the shafts and the structure as a whole when the frequency of the perturbing force approaches the eigenfrequency of the system, i.e., at resonance. The stress in the shafts then increases significantly and is mainly due not to an external force but to inertial forces in the oscillating masses. To maintain the strength of the gear system, resonance must be avoided. Hence, we see the importance of vibrational design of the structure, in which the eigenfrequencies of its components are determined and permissible speed ranges are established. The drive shafts and driven shafts of two-flow threeand five-stage modular gear systems connected to gears and two-crown gear modules have infinitely many degrees of freedom. Mathematical description of this system may be based on partial differential equations. To simplify the solution, the system with a continuous parameter distribution is replaced by a system with a discrete distribution, characterized by a finite number of degrees of freedom. The two-crown gear modules on the driving and driven shafts are assumed to be floating, weightless, and undeformable. This permits transition to a system with a point mass, which has one degree of freedom, and to description of the system’s motion using an ordinary differential equation. Obviously, both torsional and flexural oscillations are most significant for the high-speed shaft (the drive shaft) of the gear system. Vibration of this shaft is mainly associated with flexural deformation. In approximate calculations, the drive shaft with a twocrown gear module may be regarded as a rod with a point mass (disk), hinged to rigid bearings. The mass of the shaft is reduced to the mass of the gear module by summation, taking account of the reduction coefficient, which depends on the positions of the bearings and the gear module.
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