Research Article  Open Access
Zhihui Liu, Hongzhi Yan, Yuming Cao, Yuqing Lai, "Bifurcation and Chaos Analysis of the Spur Gear Transmission System for OneWay Clutch, TwoShaft Assembly", Shock and Vibration, vol. 2017, Article ID 8621514, 12 pages, 2017. https://doi.org/10.1155/2017/8621514
Bifurcation and Chaos Analysis of the Spur Gear Transmission System for OneWay Clutch, TwoShaft Assembly
Abstract
A fourdegreeoffreedom nonlinear transverse and torsional vibration model of spur gear transmission system for oneway clutch, twoshaft assembly was developed, in which the oneway clutch was modeled as a piecewise nonlinear spring with discontinuous stiffness, considering the factors such as the timevarying gear mesh stiffness, static transmission error, and nonlinearity backlash. With the help of bifurcation diagrams, time domain response diagrams, phase plane diagrams, and Poincaré maps, the effects of the excitation frequency and the torsional stiffness of oneway clutch on the dynamic behavior of gear transmission system for oneway clutch, twoshaft assembly are investigated in detail by using RungeKutta method. Numerical results reveal that the system response involves period1 motion, multiperiodic motion, bifurcation, and chaotic motion. Large torsional stiffness of oneway clutch can increase the impact and lead to instability in the system. The results can present a useful source of reference for technicians and engineers for dynamic design and vibration control of such system.
1. Introduction
The oneway clutch, twoshaft assembly is the key component of the twospeed transmission, which is widely used in loaders, helicopters, tanks, military trucks, and other gear transmission systems. The twospeed transmission is generally composed of the outer ring gear, intermediate input shaft, inner star wheel, and a plurality of cylinder rollers or sprags. The oneway clutch is made up of the outer ring gear, sprags, and the inner star wheel. The outer ring gear and the inner star wheel can be engaged or disengaged according to their relative angular speed, which can lead to the twospeed transmission having two kinds of output speed.
It is well known that gear mechanisms are widely used owing to their rather large technical advantages. However, they are known as one of the most important sources of vibration and noise in mechanical transmission systems. The vibration, noise, and wear performances are mainly affected by the gear pair dynamic characteristics.
There is a growing literature on nonlinear dynamics of gear pairs in the past decades. And to analyze the nonlinear dynamic behaviors of gear transmission system, the different excitation of static transmission error, dynamic meshing stiffness, bearing contact stiffness, prime mover, clearance nonlinearity, and load fluctuation are added [1–7]. Walha et al. [8] investigated the dynamics of a twostage gear system with mesh stiffness and backlash. Parker et al. [9] used a finite element/contact mechanic model to investigate the dynamic response of a spur gear pair. And the dynamic characteristics of a gear pair are analyzed across a wide range of frequency and torques. AlShyyab and Kahraman [10] adopted lumped parameter method to establish a nonlinear timevarying dynamic model for multimesh gear, considering the nonlinear gear gap and gear meshing stiffness. The multiterm harmonic balance method (HBM) was used to gain the steadystate period1 response, including the Root Mean Square (RMS) and the mean value of the vibration amplitude across a wide range of frequency, taking into account different gear meshing stiffness. He et al. [4] analyzed the dynamic characteristics of a spur gear pair, considering the dynamic meshing stiffness and sliding friction. The influence of friction on dynamic transmission error is discussed. In recent years, many scholars have studied the bifurcation and chaos characteristics of gear transmission system [11]. Wang et al. [12] made use of the bifurcation diagrams, phase plane diagrams, Poincaré maps, time domain response diagrams, and amplitudefrequency spectrums to investigate the effects of the pinion speed and stiffness on the dynamic behavior of gear transmission system for locomotive. Xiang et al. [13] built a sixdegreeoffreedom nonlinear dynamic model of a spur gearbearing system with timevarying stiffness, gear backlash, and surface friction. In [13], bifurcation diagrams of the mesh stiffness and the rotational speed ratio as control parameters were used to observe the dynamic orbits of the system. The chaotic motion was identified from the largest Lyapunov exponents, Poincaré maps, and the phase diagrams of the system. ChangJian and Chang [14] studied the dynamic orbits of a singledegreeoffreedom spur gear system by using bifurcation diagrams with the dimensionless damping coefficient and the dimensionless rotational speed ratio as control parameters. Gou et al. [15] used the simple cell mapping method and escape time algorithm to examine the bifurcation dynamic characteristics of the multiparameter coupling in torsionvibration gear system. Although most scholars study the steadystate response analysis of gear transmission system, Khabou et al. [16] studied a spur gear dynamic behavior in the transient regime.
The dynamic analysis of oneway clutch, twoshaft assembly is to study the coupling nonlinear characteristics of oneway clutch and gear transmission system. Though application of oneway clutch, twoshaft assembly is extensive, literature on its dynamics is limited. In the aspects of dynamic characteristics study of oneway clutch, Vernay et al. [17] pointed out and quantified the possible relative sliding effects between spragtype races of oneway clutches by experiments. GillJeong [18] verified the nonlinear behavior analysis of a paired spur gear system with a oneway clutch for the first time. He found that the dynamic transmission error of a gear system with a oneway clutch was reduced over the entire frequency range compared to a pure gear system with threedegreeoffreedom torsional vibration model. However, the effects of parameters such as bearing stiffness, bearing backlash, torsion stiffness, and damping of clutch on the nonlinear behavior of gear system coupled with a oneway clutch were not considered. In order to investigate the effect of the oneway clutch on the dynamic performance of the coupling transmission, a great deal of research effort has been devoted to the study of the nonlinear dynamics of oneway clutches in beltpulley systems. In such system, the oneway clutch is usually modeled as a twodegreeoffreedom model, which is regarded as piecewise linear [19]. Zhu and Parker [20] used a twodegreeoffreedom model to examine the nonlinear dynamics of a twopulley belt system with a oneway clutch through three methods of multiterm harmonic balance, numerical integration, and the bifurcation software AUTO separately. Zhu and Parker [21] also used the method of multiple scales to obtain the periodic solutions of a twopulley belt system with clearancetype nonlinearity. The stable steadystate periodic responses of a beltdrive system with a oneway clutch were studied comprehensively [22–25]. Ding and Zu [22] studied the effects of the system parameters on the nonlinear steadystate response of a beltdrive system with a oneway clutch and had a conclusion that oneway clutch not only decreases the resonance amplitude of the driven pulley and shaft’s rotational vibration but also reduces the resonance region of the belt’s transverse vibration. Ding [23] also presented the stable steadystate periodic response of a twopulley beltdrive system coupled with oneway clutch under double excitation for the first time. The Galerkin method was adapted to exam whether the oneway device can efficiently reduce the rotation vibration and transverse vibration of the pulley belt dynamic system either.
In view of the lack of research for dynamic analysis for oneway clutch, twoshaft assembly, the present paper concentrates on building and analyzing a mathematical model for such system. For the first time, a fourdegreeoffreedom nonlinear transverse and torsional vibration model of spur gear transmission system for oneway clutch, twoshaft assembly was modeled, considering the gear masses and , a nonlinear mesh stiffness , and mesh damping . The oneway clutch is modeled as a piecewise nonlinear spring with discontinuous stiffness that separates the driven gear into two degrees of freedom. The main purpose is to inspect the influences of the gear speed and the torsional stiffness of oneway clutch on the system dynamic behavior and find out some useful reference information for technicians and engineers to dynamic design and vibration control of such system.
2. Working Principle of OneWay Clutch, TwoShaft Assembly
Figure 1 shows the structural schematic of oneway clutch, twoshaft assembly, which is composed primarily of bearing (1, 2), gear (1, 2), sprags, input shaft, output shaft, and inner ring. Gear 1 is fixed on the input shaft by the method of spline interference fit. Gear 2, sprags, and the inner ring, which is connected to the output shaft through key connection, are formed into a oneway clutch. Figure 2 is used as a reference to explain the work principle of the oneway clutch. When the oneway clutch is not working, the tension of the spring ensures that the sprags keep in touch with gear 2 and the inner ring. When gear 2 begins to rotate clockwise under the action of gear 1 or the rotation speed of gear 2 exceeds the rotation speed of the inner ring, the sprag will rotate around its center in clockwise direction with the spring tension and the tangential friction at the contact point. With the sprag rotating, the distance of the two contact points between the sprag and gear 2 and the inner ring would become longer, and the power can be transmitted from gear 2 to the inner ring. As gear 2 and the inner ring are fully wedged by the sprags, the rotation speed of gear 2 and the inner ring will be the same. Conversely, gear 2 will be overrunning and the power could not be transmitted to the inner ring when gear 2 rotates anticlockwise or the rotation speed of gear 2 is slower than the rotation speed of the inner ring. So it can be concluded that the rotation direction of gear 1 determines whether the load can be transferred for the oneway clutch, twoshaft assembly.
3. Mathematical Model
Figure 3 shows a schematic illustration of the dynamic model of oneway clutch, twoshaft assembly considered in the present analysis. In this model, is the base circle radius of gear 1, is the base circle radius of gear 2, is the mass moments of inertia of gear 1, is the mass moments of inertia of gear 2, is the mass moment of inertia of inner ring, is the mass of gear 1, is the mass of gear 2, is the damping coefficient of the gear mesh, is the timevarying stiffness coefficient of the gear mesh, which can be obtained by assuming a rectangular wave as shown in (2) [8, 18], where is the average mesh stiffness value, and are the th Fourier coefficient and phase angle of , respectively, and , is the involute contact ratio, , is the forcedisplacement on the mesh line function of gear mesh, is the damping coefficient of bearing 1, is the damping coefficient of bearing 2, , are the contact stiffness coefficient and the forcetransverse displacement function of th bearing , is the torsional stiffness coefficient of oneway clutch, and is the torsional damping coefficient of oneway clutch. From the lumped parameter mass method and Newton’s laws of motion, the fivedegreeoffreedom nonlinear model of the geared clutch bearing system dynamic model can show that where gear 1 and gear 2 are assumed perfect involute spur gears with no modifications and the torsional and transverse flexibility of the input shaft and output shaft are neglected. Here, and are the transverse and torsional displacements of the th gear (), is the torsional displacement of the inner ring, and means derivative with respect to time . The input torque is assumed to be fluctuating as , where is the average torque and is the fluctuating torque, considered as . Forcing term , which is connected with the piecewise nonlinear forcedisplacement function shown in (4), and forcevelocity function [26], is the torque transferred from gear 2 to the inner ring, as shown in (3). And the output torque applied on the inner ring or output shaft is assumed to be constant: that is, . The external radial forces and are preloads which are applied to both rolling element bearings. The static transmission error , connected with the manufacturing and assembling of the gears, is considered sinusoidal excitation as
It is assumed that , , and , where the parameters of , , and are defined as the displacement on the direction of mesh line of gear 1, gear 2 and the inner ring, respectively. Through defining new variables and as and , (1) can be simplified further as
Here, is the equivalent gear pair mass. The piecewise linear displacement functions and include the half of backlash of bearings and the half of backlash of the gears , which can be expressed as (7) and (8).
A dimensionless form of (5) can be obtained by letting where is the characteristic length and the terms and are the fundamental excitation frequencies of external torque fluctuations and the internal static transmission error, respectively. And the dimensionless governing equations of motion are shown as (10), where is the dimensionless transverse displacement of the th gear , is dimensionless difference between the dynamic transmission error and the static transmission error of the two gears, and is the dimensionless dynamic transmission error between gear 2 and the inner ring.
4. Parametric Studies on Characteristics of Bifurcation and Chaos
In this section, a case study is analyzed to demonstrate the effect of the rotation speed of gear 2 and the torsional stiffness of oneway clutch on its dynamic characteristics.
For the structure of oneway clutch, twoshaft assemblies, gear 2 and the inner ring can be coupled or decoupled as the oneway clutch is active.
The main parameters of the oneway clutch, twoshaft assemblies are listed in Table 1. Equation (10) describes a strongly nonlinear dynamic system with timevarying gear mesh stiffness, nonlinear backlash, and nonlinear forcedisplacement function of oneway clutch. And it is solved by using the fourthorder RungeKutta method. In order to obtain a better understanding of the dynamic behavior of the oneway clutch, twoshaft assembly, the time series data were used to generate the bifurcation diagram, phase diagram, and Poincaré maps. The periodic responses are shown by varying the excitation frequency and the torsional stiffness of oneway clutch. On the other hand, since the new introduced coordinates z_{1} and z_{2} have the similar nonlinear behavior, the dynamic response of the transverse vibration z_{2} of gear 2 is selected to analyze the bifurcation and chaos characteristics. In order to find out the dynamic response of the windup angle of oneway clutch, the character of dynamic transmission error between gear 2 and the inner ring is chosen to be analyzed. Furthermore, in order to avoid the risk of obtaining transient solutions and minimize computing, the initial conditions of , , , , , and are all set to be zero.

4.1. Effect of Excitation Frequency
The ratio of the bearing stiffness to average gear mesh stiffness is introduced to represent the change of support stiffness. The frequency parameter is assigned as control parameters. The bifurcation diagram of the dimensionless transverse displacement of gear 2 with excitation frequency change is presented in Figure 4.
It is well known that the jump phenomenon usually exists in the dynamic response of nonlinear system. It could be seen clearly in Figure 4 that there is a phenomenon of jumping at value of . The oneway clutch, twoshaft assemblies system mainly exhibits periodone motion at low values or at high excitation frequency: that is, or . Just as shown in Figure 5(a), the time domain response diagram is a sine wave, the phase plane diagram is only one closed circle, and the Poincaré map is a single point. It is observed that the system goes into chaotic region within the range of , and . It can be seen in Figure 5(b) that the time domain response diagram shows a nonperiodic motion, the phase plane diagram is disorder, and the Poincaré map shows many discrete points. As is increased from 0.88 to 0.93 and from 1.14 to 1.19, the system exhibits unstable periodone motion, and the period2 motion will be observed over the range of . And as it is shown in Figure 5(c), the time domain response diagram shows a period motion, the phase plane diagram shows two closed circles, and the Poincaré map shows two unique points. Figure 5 presents time series, phase plane diagram, and Poincaré maps of Hopf bifurcation points at , 0.7, 1.2, 1.3, 1.6, and 1.63. It can be seen that the motions of the oneway clutch, twoshaft assemblies system undergo period1 motion, chaotic motion, period2 motion, quasiperiodic motion, and period7 motion.
(a)
(b)
(c)
(d)
(e)
(f)
Figure 6 presents the bifurcation diagram of the system response of dimensionless dynamic transmission error between gear 2 and the inner ring, which is essentially used to study the dynamic windup angle of oneway clutch, using excitation frequency as control parameter. It can be observed that the relative reverse motion between gear 2 and the inner ring exhibits rather complex phenomenon with the increase of the excitation frequency . There exists some “frequency hopping” at , 0.29, and 0.61, where the system undergoes the transient transition between periodone motion. Only periodone motion can be observed at low values of the excitation frequency, that is, , or at high values of the excitation frequency, that is, . The system performs period2 motion within the range of . The system exhibits chaotic motions within the range of , , and . Unlike the transverse motion of gear 2, the relative reverse motion between gear 2 and the inner ring exhibits stable period1 motion within the range of , . The system goes into chaotic motions through the quasiperiodic route around excitation frequency points , 0.931, and 1.31 and goes into chaotic motions through the quasiperiodic route around excitation frequency points , 1.141, and 1.681.
Figure 7 shows the time series, phase plane diagram, and Poincaré maps of Hopf bifurcation points at , 0.7, 1.2, 1.3, 1.6, and 1.63. It can be founded that the system behavior undergoes period1 motion, chaotic motion, period2 motion, quasiperiodic motion, and period7 motion with the increase of the excitation frequency .
(a)
(b)
(c)
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4.2. Effect of Torsional Stiffness of OneWay Clutch
Figure 8 presents the bifurcation diagram of the system response of dimensionless dynamic transmission error between gear 1 and gear 2, using the torsional stiffness of oneway clutch as control parameter. It can be observed from the figure that, when the torsional stiffness is changed, there exist kinds of motion forms, such as periodic1 motion, periodic2 motion, periodic4 motion, periodic8 motion, and chaotic motion. In order to accurately distinguish the motion form, the time domain response diagrams, phase plane diagrams, and Poincaré maps are listed to illustrate the dynamic characteristics of the system in Figure 9. When is less than 276000 N·m/rad, only periodone motion can be observed. The system motion state will be changed from periodic1 motion to periodic2 motion, when the torsional stiffness of oneway clutch is increased to 276000 N·m/rad, and the state is continued until 331000 N·m/rad. The system performs the transient periodic4 motion within the range of 331000 N·m/rad ≤ ≤ 341000 N·m/rad and exhibits chaotic motions within the range of 341000 N·m/rad ≤ ≤ 676000 N·m/rad, just as shown in Figure 9(c). It can be seen that the time domain response diagram shows a nonperiodic motion, the Poincaré map shows many discrete points, and the phase plane diagram is disorder. With the increasing of the torsional stiffness, the system leaves chaos and goes into periodic8 motion from 676000 N·m/rad to 696000 N·m/rad. When the torsional stiffness is greater than 696000 N·m/rad, the system goes into another region of chaotic motion again until 811000 N·m/rad. After undergoing the chaotic region, the system leaves chaotic motion and goes into periodic1 motion again within the range of 811000 N·m/rad ≤ ≤ 951000 N·m/rad. When is higher than 951000 N·m/rad, the system leaves periodic1 motion and returns into chaotic motion again.
(a)
(b)
(c)
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5. Summary and Conclusions
A general multidegreeoffreedom nonlinear dynamic model of oneway clutch, twoshaft assembly based on lumped parameter method (LPM) is proposed in this paper. The gear backlash, bearing backlash, a nonlinear mesh stiffness , and mesh damping are considered in the model. The oneway clutch is modeled as a piecewise nonlinear spring with discontinuous stiffness that separates gear 2 into two degrees of freedom. The dynamic response of oneway clutch, twoshaft assemblies is studied over a wide range of frequencies. Speed sweeping is used to check the effect of oneway clutch on the nonlinear behavior of gear transmission system, by applying variable stepsize RungeKutta method.
As mentioned above, with the increasing of excitation frequency and torsional stiffness of oneway clutch, the system of oneway clutch, twoshaft assembly is prone to involve periodic1 motion, multiperiodic motion, and chaotic motion. Large torsional stiffness of oneway clutch can increase the impact and lead to instability in the system. To reduce the impact and increase stability, the excitation frequency of the engine and the torsional stiffness of the oneway clutch are taken into account to be based on matching and optimization principles for the system of oneway clutch, twoshaft assembly.
Nomenclature
:  Base circle radius of gear 1 
:  Base circle radius of gear 2 
:  Mass moment of inertia of gear 1 
:  Mass moment of inertia of gear 2 
:  Mass moment of inertia of inner ring 
:  Mass representing inertia of gear 1 
:  Mass representing inertia of gear 2 
:  Mass representing inertia of inner ring 
:  Equivalent gear pair mass 
:  Viscous damping coefficient of bearing 1 
:  Viscous damping coefficient of bearing 2 
:  Viscous damping coefficient of gear pair 
:  Torsional damping of oneway clutch 
:  Contact stiffness of bearing 1 
:  Contact stiffness of bearing 2 
:  Timevarying mesh stiffness of gear pair 
:  Torsional stiffness of oneway clutch 
:  Forcedisplacement function of bearing 1 
:  Forcedisplacement of bearing 2 
:  Nonlinear displacement function of gear pair 
:  Preload applied on bearing 1 
:  Preload applied on bearing 2 
:  Force transmitted through oneway clutch 
:  Torque acting on gear 1 
:  Torque acting on gear 2 
:  Torque acting on inner ring 
:  Average torque acting on gear 1 
:  Fluctuating torque acting on gear 1 
:  Transverse displacement of gear 1 
:  Transverse displacement of gear 2 
:  Displacement on direction of mesh line of gear 1 
:  Displacement on direction of mesh line of gear 2 
:  Displacement on direction of mesh line of inner ring 
:  Torsional displacement of gear 1 
:  Torsional displacement of gear 2 
:  Torsional displacement of inner ring 
:  Static transmission error 
:  The half of backlash of bearing 1 
:  The half of backlash of bearing 2 
:  The half of backlash of the gear pair 
:  The characteristic length 
:  Excitation frequency of static transmission error 
:  Excitation frequencies of external torque 
:  Natural frequency 
:  Involute contact ratio 
:  Dimensionless transverse displacement of gear 1 
:  Dimensionless transverse displacement of gear 2 
:  The dimensionless difference between the dynamic transmission error and the static transmission of the gear pair 
:  The dimensionless difference of the displacement on direction of mesh line of gear 2 and the displacement on direction of mesh line of inner ring of oneway clutch 
:  The difference between the dynamic transmission error and the static transmission () of the gear pair 
:  The difference of the displacement on direction of mesh line of gear 2 and the displacement on direction of mesh line of inner ring of oneway clutch. 
Conflicts of Interest
The authors declare that there are no conflicts of interest regarding the publication of this paper.
Acknowledgments
The authors thank the Key Research and Development Program in Hunan Province (no. 2015JC3007), the Basic Research on Digital Machining of Hard Processed Aeronautical Parts (no. 2011CB706800), and General Project in Hunan Province Department of Education (no. 15c1239) for financial support.
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Copyright
Copyright © 2017 Zhihui Liu et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.