Abstract

Due to the energy crisis and global warming issues, the wind energy is becoming one of the most attractive renewable energy resources in the world. The drivetrains in the wind turbine tend to fail more prematurely than those in any other applications. Gearbox is the subsystem that causes the most downtime for the wind turbines. In the previous research, only the torsional flexibility of the shaft was considered in the drivetrain model. However, because the shaft is longer than other parts, and components connected by the shaft affect each other via shaft bending, the flexibility of the shaft cannot be ignored. In this study, a spherical joint that consists of three rotational springs was used to define the shaft bending. This shaft bending will affect the drivetrain rotation, the translational motion and the gear mesh contact force. Additionally, the eccentricity and the nacelle movement are analyzed due to the coupled motion. In this paper, a mathematical model of the drivetrain is proposed, which is a three-dimensional dynamic model that includes flexible bearings, a gear mesh model, shaft flexibility, eccentricity, and nacelle movement. The equation of motion of the drivetrain is derived using Lagrange's equation. The governing equation is solved numerically via direct numerical integration. The dynamic responses of the system and contact forces between the gear tooth in the time and frequency domains are calculated numerically. The study shows that this dynamic model of the drivetrain will be highly useful for subsequent studies on the wind turbine condition monitoring.

Highlights

  • Due to the energy crisis, many countries are attempting to exploit various renewable energies

  • Multibody Dynamic Analysis of a Wind Turbine Drivetrain all the components of wind turbines, high failure rates of gearbox components have been observed in the wind industry since its inception (Bhardwaj et al, 2019)

  • The magnitudes of vibration are increasing through the drivetrain due to the gear ratio

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Summary

INTRODUCTION

Due to the energy crisis, many countries are attempting to exploit various renewable energies. He et al (2019) applied the time varying mesh stiffness for two-stagespur gear model considering the gear eccentricity. The shaft bending, eccentricity, nacelle movement and varying gear mesh are taken into account in this model. In the previous study (Shi et al, 2013), each component has one DOF, and only the torsional stiffness of the shaft and the gear mesh are considered based on the rotational coordinates. The gear mesh stiffness is defined as a function of the varying angular displacement with the eighth-order Fourier series (Eq 6). This model will be used in the present study. The rotor is exited with an angular velocity of 6 rpm

RESULTS AND DISCUSSION
DATA AVAILABILITY STATEMENT
CONCLUSION

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