Abstract
In light of ignoring the effect of backlash on mesh stiffness in existing gear dynamic theory, a precise profile equation was established based on the generating processing principle. An improved potential energy method was proposed to calculate the mesh stiffness. The calculation result showed that when compared with the case of ignoring backlash, the mesh stiffness with backlash had an obvious decrease in a mesh cycle and the rate of decline had a trend of decreasing first and then increasing, so a stiffness coefficient was introduced to observe the effect of backlash. The Fourier series expansion was employed to fit the mesh stiffness rather than time-varying mesh stiffness, and the stiffness coefficient was fitted with the same method. The time-varying mesh stiffness was presented in terms of the piecewise function. The single degree of freedom model was employed, and the fourth order Runge–Kutta method was utilized to investigate the effect of backlash on the nonlinear dynamic characteristics with reference to the time history chart, phase diagram, Poincare map, and Fast Fourier Transformation (FFT) spectrogram. The numerical results revealed that the gear system primarily performs a non-harmonic-single-periodic motion. The partially enlarged views indicate that the system also exhibits small-amplitude and low-frequency motion. For different cases of backlash, the low-frequency motion sometimes shows excellent periodicity and stability and sometimes shows chaos. It is of practical guiding significance to know the mechanisms of some unusual noises as well as the design and manufacture of gear backlash.
Highlights
Gear dynamics is an important method to predict dynamic performance as well as to monitor the status of a gear system
The time-varying mesh stiffness caused by alternately changing the gear pairs in mesh plays a crucial role in dynamic responses
Potential energy method always ignore the influence of backlash on mesh stiffness
Summary
Gear dynamics is an important method to predict dynamic performance as well as to monitor the status of a gear system. One consistently popular topic in gear dynamics is how to describe the change rule of time-varying mesh stiffness correctly and effectively. In References [2,3,4], time-varying mesh stiffness was simplified as a rectangular equation which had significant differences from the actual value. Yang proposed an equation the single mesh tooth stiffness in Reference gear [6]. Tang revised calculation formula and proposed an analytical method to calculate the Chen mesh considering the Kuang’s load condition and the tooth profile modification in References. Chen investigated the differences between the rectangular stiffness and its approximate form on nonlinear dynamic characteristics in Reference [11]. The FEM and potential energy method always ignore the influence of backlash on mesh stiffness. As well as direct the design and control of the gear’s backlash
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