Abstract

The aim of this research was to design a physically consistent model for the forced torsional vibrations of automotive driveshafts that considered aspects of the following phenomena: excitation due to the transmission of the combustion engine through the gearbox, excitation due to the road geometry, the quasi-isometry of the automotive driveshaft, the effect of nonuniformity of the inertial moment with respect to the longitudinal axis of the tulip–tripod joint and of the bowl–balls–inner race joint, the torsional rigidity, and the torsional damping of each joint. To resolve the equations of motion describing the forced torsional nonlinear parametric vibrations of automotive driveshafts, a variational approach that involves Hamilton’s principle was used, which considers the isometric nonuniformity, where it is known that the joints of automotive driveshafts are quasi-isometric in terms of the twist angle, even if, in general, they are considered CVJs (constant velocity joints). This effect realizes the link between the terms for the torsional vibrations between the elements of the driveshaft: tripode–tulip, midshaft, and bowl–balls–inner race joint elements. The induced torsional loads (as gearbox torsional moments that enter the driveshaft through the tulip axis) can be of harmonic type, while the reactive torsional loads (as reactive torsional moments that enter the driveshaft through the bowl axis) are impulsive. These effects induce the resulting nonlinear dynamic behavior. Also considered was the effect of nonuniformity on the axial moment of inertia of the tripod–tulip element as well as on the axial moment of inertia of the bowl–balls–inner race joint element, that vary with the twist angle of each element. This effect induces parametric dynamic behavior. Moreover, the torsional rigidity was taken into consideration, as was the torsional damping for each joint of the driveshaft: tripod–joint and bowl–balls–inner race joint. This approach was used to obtain a system of equations of nonlinear partial derivatives that describes the torsional vibrations of the driveshaft as nonlinear parametric dynamic behavior. This model was used to compute variation in the natural frequencies of torsion in the global tulip (a given imposed geometry) using the angle between the tulip–midshaft for an automotive driveshaft designed for heavy-duty SUVs as well as the characteristic amplitude frequency in the region of principal parametric resonance together the method of harmonic balance for the steady-state forced torsional nonlinear vibration of the driveshaft. This model of dynamic behavior for the driveshaft can be used during the early stages of design as well in predicting the durability of automotive driveshafts. In addition, it is important that this model be added in the design algorithm for predicting the comfort elements of the automotive environment to adequately account for this kind of dynamic behavior that induces excitations in the car structure.

Highlights

  • In Feng, Rakheja, and Shangguan [8], optimization of the generated axial force (GAF) of a driveshaft system with the interval of uncertainty was treated without considering the CVJ isometry of the driveshaft, which is no longer isometric, and this aspect has been certified by experiments using the vertex method for analysis of the upper and lower bond (ULB) variation in parameters

  • The tulip in torsional rigid body movement reduced to the torsional longitudinal axis of the midshaft, having a global torsional stiffness ktGT, a global torsional damping coefficient ctGT, an axial geometric moment of inertia of the cross section for the global tulip JX2 GT reduced to the longitudinal axis of the midshaft in the centroid of the cross section of tripode fixed on the midshaft (see Equation (1)), an axial mass moment of inertia of the cross section for the global tulip IX2 GT reduced to the longitudinal axis of the midshaft in the centroid of the cross section of tripode fixed on the midshaft (see Equation (5)), where ktGT and ctGT are given by the equations: ktGT =

  • Midshaft of the driveshaft that is quasi-isometric for the angular velocity φ3 [1,4], the effect of the impulsive reaction moment from the wheels [3], the effect of nonuniformity on the axial moment of inertia of the joint that varies with the angle φ3, the effect of nonuniformity on the axial moment of inertia of the global bowl that varies with the angle φ3, the effect of the angle β2 between the global bowl axis and the midshaft axis, and the effect of the torsional rigidity as well as the torsional damping for the joint bowl–inner race–midshaft of the driveshaft that are functions of the angle φ3

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Summary

Introduction

The present work presents a consistent model to describe the forced torsional vibrations of an automotive driveshaft considering the following aspects: the joints of the driveshaft are quasi-isometric in terms of angular velocity [1] even if they are generally considered to be CVJs (constant velocity joints); the effect of induced torsional loads such as the harmonic entry moment from the gearbox [2] (p. 360) and the impulsive reaction moment from the wheels [3]; the effect of nonuniformity on the axial moment of inertia of the joints that varies with the angle of twist of each element of the driveshaft, and the effect of the torsional rigidity as well as the torsional damping for each joint of the driveshaft, which varies with the angle of twist of each element of the driveshaft. The present work presents a consistent model to describe the forced torsional vibrations of an automotive driveshaft considering the following aspects: the joints of the driveshaft are quasi-isometric in terms of angular velocity [1] even if they are generally considered to be CVJs (constant velocity joints); the effect of induced torsional loads such as the harmonic entry moment from the gearbox [2] CVJ The quasi-homokinetic driveshaft model that includes dynamic elementsmodel describing nonlinear goal of this study was to establish a complete for be anthe automotive forced parametric dynamic behavior. It isthat envisaged that this model can be used in the quasi-homokinetic driveshaft model includes elements describing the nonlinear early stages of design as well as in predicting the durability of automotive driveshafts.

Schematic representation ofthe an axes automotive
Computation of the Mass Moments and Geometric Moments of Driveshaft Inertia
The Equations of Forced Torsional Vibrations of the Automotive Driveshaft
The Mathematical Procedure Solution
Case Study Analysis of Principal Parametric Resonance of the Global Tulip
Results and Discussions

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