Stability and bifurcation of a flexible rodfastening rotor bearing system with a transverse open crack
Nanshan Wang^{1} , Heng Liu^{2} , Yi Liu^{3} , Zhidong Xu^{4}
^{1, 2, 3, 4}School of Mechanical Engineering, Xi’an Jiaotong University, Xi’an, 710049, China
^{1, 2, 3, 4}Key Laboratory of Education Ministry for Modern Design and RotorBearing System, Xi’an Jiaotong University, Xi’an, 710049, China
^{2}Corresponding author
Journal of Vibroengineering, Vol. 20, Issue 8, 2018, p. 30263039.
https://doi.org/10.21595/jve.2018.19429
Received 17 November 2017; received in revised form 4 June 2018; accepted 22 June 2018; published 31 December 2018
JVE Conferences
The stability and bifurcation of a flexible rodfastening rotor bearing system with a transverse open crack in a fastening rod are investigated. The nonlinear dynamic model of a cracked rodfastening rotor system is established based on the finite element method. A methodology is introduced where shooting method, pathfollowing technique, and Floquet theory are combined for determining the periodic solutions and stability margins of the system. The effects of crack depth and mass eccentricities on the system are studied by numerical simulations. Results show the system stability will reduce due to the presence of crack, two saddlebacks occur on the periodicdoubling borderline whose bottom location corresponds to the two resonant peak of bearing node, and effects of the crack and mass eccentricity play a dominant position in different conditions respectively. Comparisons between the cracked rotor system and the intact ones referred in the literature indicate that some special characteristics of cracked rodfastening rotor system in motion orbits and frequency components can be used to detect the presence of crack and its depth.
 The model of rodfastening rotor system with a crack in a fastening rod are developed.
 The presence of crack in a rod leads to the reduction of the system stability.
 Two resonant peak can be found in the cracked rodfastening rotor system.
 The effects of crack play a dominant position for balanced rodfastening rotor system.
 Periodicdoubling bifurcation early occurs to cracked system for small mass unbalance.
Keywords: dynamics, stability, bifurcation, crack, rodfastening rotor system.
1. Introduction
The stability and bifurcation of cracked rotor bearing system have always been the focus of attention. The fatigue crack is a very typical failure of rotor bearing system, which always causes great damage to some extent. It is essential to find out the dynamic characteristics of rotor system at the initial stage of crack and take appropriate measures in time to avoid some serious losses, especially for complex rodfastening rotor bearing system. Rodfastening rotor bearing system is a kind of typical structural pattern of combined rotor system in which always more than two disks are fastened by one central rod or several circumferentially distributed rods. It widely exists in gas turbine, aircraft engine and power generation which occupy a dominant position in modern heavy industrial equipment. When there is a crack in a rotor spindle, a fastening rod or a disk of the rodfastening rotor system, the dynamic behaviours of the system will become complicated compared with Jeffcott rotor system and the destructive effect is even more catastrophic in a sort of way.
During the past several decades, for the dynamic behaviours of cracked rotor bearing system, many studies have been carried out theoretically or experimentally [114]. Most of their studies based on the Jeffcott rotor system and rotor shaft crack. Meanwhile, the dynamics of cracked rotor system with different structures have been attracted more attentions gradually and many of them didn’t contain the fastening rods. The effects of a transverse crack on the dynamics of a multirotor, multibearing system [15] or a fragment of the shaft of constant crosssection system with considering the coupled torsional and bending vibrations [16] are carried out, respectively. ALShudeifat [17, 18] obtained the timevarying stiffness of cracked rotor and investigated the stability of cracked rotor bearing system with two disks. Han and Chu [19] investigated the effect of a transverse crack on the parametric instability of a rotorbearing system with two disks, and one of them is asymmetric. Nagata and Inoue [20] developed an analytical method to detect the vibration behaviours of cracked rotor bearing system with three disks. Bala Murugan [21] conducted considerable analyses of cracked rotor bearing system with multidisk and variable cross section. Their studies provided many useful strategies for treating the problem of cracked rotor bearing system especially for complex rotor systems. Whether it is the Jeffcott rotor or other complex rotor system mentioned above, they are not attached to any fastening rod. It is this typical structure between rodfastening rotor system and nonrod fastening rotor system that makes some differences in dynamic behaviours. For nonrodfastening rotor system, the corresponding dynamic models are developed based on condition that the system gravity occupies a domain position. While this assumption of dominant gravity can’t directly be used for the rodfastening rotor system because the big tension stress of fastening rod far outweighs the compressive stress and additional bending stress caused by the system gravity. Meanwhile, it is worth noting that this will lead to this kind of rodfastening rotor system working in an opening crack mode mostly. Besides, because of the alternating stress of system, a fatigue crack either in a rod or a disk become easy to appear on the direct contact position between the fastening rod and disk as well as in the vicinity of this position. While the crack is on shaft or fastening rod, the dynamic behaviours especially the nonlinear dynamic behaviours of system have not gained sufficient attentions.
In order to reflect the dynamic behaviours of the rodfastening rotor bearing system with cracks and consider the big tension stress effects of the fastening rod, the nonlinear dynamic model of the system with a transverse open crack in a fastening rod is developed based on the finite element method. A combined technique is employed to investigate the system stability and bifurcation.
2. Modeling of cracked rodfastening rotor bearing system
2.1. Dynamic modeling of a fastening rod with no crack
The flexible rodfastening rotor bearing system is depicted in Fig. 1. Four rigid disks, mounted on the rotor shaft, are fastened by several circumferentially distributed rods and the rotor is supported by two radial cylindrical bearings. The rotor shaft is discretized by using the finite element method with Timoshenko beam, and then the attached fastening rod are modeled as spring element with no mass. The notations as illustrated in Fig. 1 and other essential physical parameters are given in Table 1.
Fig. 1. Flexible rodfastening rotor bearing system. The labels ‘a’, ‘b’, ‘c’, and ‘d’ denote the four disks for distinguishing
The modeling of a fastening rod with no crack as explained in [22, 23] is briefly presented. The instantaneous tension of each rod as shown in Fig. 1 is determined by the position of rod both ending points, which are located on the corresponding disks ‘a’ and ‘d’. According to [22, 23], the elongation and axial force of $i$th fastening rod due to the vibration of rotor system can be expressed approximately as follows:
where ${\phi}_{a}$, ${\phi}_{d}$, ${\psi}_{a}$,$\mathrm{}$and ${\psi}_{d}$ are the tilting angles. $\omega $ is the rotating speed of the rotor. $r$ is the radius of distributed circumference of the n rods. where ${\gamma}_{i}$ is the mounted angle of $i$th fastening rod and this rods are distributed averagely with ${\gamma}_{i}=2\pi i/n$ ($i=$1, 2, …, $n$, $n$ ≥ 3). ${F}_{0}^{i}$, $L$, and $A$ is the pretightening force, the original length and the crosssection area of the fastening rod, respectively.
Table 1. Material properties and geometric parameters of rotor system
Parameters

values

Parameters

values

Mass density, $\rho $ (kg.m^{3})

7800

Mass eccentricities of disks, $e$ (m)

02×10^{5}

Young's modulus, $E$ (GPa)

210

Diameter of rods, ${d}_{rod}$ (m)

0.01

Poisson ratio, $\nu $

0.3

Number of rods, $n$

12

Diameter of shaft, ${d}_{s}$ (m)

0.08

Diameter of circumference of rods, ${D}_{r}$ (m)

0.12

Length of shaft, ${l}_{s}$ (m)

1.1

Pretightening load of each rod, ${F}_{0}$ (N)

15700

Diameter of disks, ${d}_{d}$ (m)

0.16

Span of two bearing, ${l}_{b}$ (m)

0.9

Width of disks, ${l}_{d}$ (m)

0.08

Width of bearing, $B$ (m)

0.08

Then the potential energy of $i$th rod is calculated as the following:
Thus, the total potential energy with $n$ fastening rods distributed along the circumference averagely can be given as:
Substituting the Eq. (1) into Eq. (4) and according to the geometrical relationship, the Eq. (4) can be expressed as follows:
with$a=r\sum _{i=1}^{n}{F}_{0}^{i}\mathrm{s}\mathrm{i}\mathrm{n}\left(\omega t+{\gamma}_{i}\right)$, $b=r\sum _{i=1}^{n}{F}_{0}^{i}\mathrm{c}\mathrm{o}\mathrm{s}\left(\omega t+{\gamma}_{i}\right)$, $c=nEA{r}^{2}/2L$, and the constant stiffness matrix ${\mathbf{K}}_{rod}$ as followed in Eq. (6):
In fact, in Eq. (5), the first term is caused by the generalized moment of the pretightening force, the second term is regarded as the dynamic stiffness term. When the pretightening forces for per rod is equal (${F}_{0}^{i}=const$ and $a=b=$ 0), the $n$ rods only provide a constant stiffness matrix ${\mathbf{K}}_{rod}$, and in contrast with an addon moment vector ${\mathbf{f}}_{rod}$ as shown in Eq. (7) besides stiffness matrix ${\mathbf{K}}_{rod}$:
2.2. Dynamic model of the fastening rod with a transverse open crack
Because per fastening rod is mainly subjected to the axial big tension stress due to the pretightening assembling, which far outweighs the compressive stress and additional bending stresses caused by the system gravity. This will determine the open crack state of cracked rod in practical work when there is a crack in a fastening rod. Besides the contact edge position of disk and fastening rods always introduces the phenomenon of stress concentration. When there is a transversal open crack on the surface of a fastening rod in “1” location as depicted in Fig. 1, it always introduces the phenomenon of stress concentration and the reduction of stiffness, and the stability of the whole rotor bearing system will change compared with intact ones (which has no crack on the fastening rod). The schematic of a transversal open crack in a fastening rod is illustrated in Fig. 2.
Fig. 2. The crosssection area of the cracked fastening rod, where $h$, ${r}_{0}$ and $\alpha $ are the depth of crack, the radius of the fastening rod and the semicentral angel corresponding to the half width of a transverse crack, respectively
When a transverse open crack occurs on the surface of the $j$th fastening rod, the crack section area and the instantaneous axial force of $j$th rod can be derived respectively as follows:
with $\lambda =h/{r}_{0}$.
Substituting the Eq. (8) into the Eq. (9), the instantaneous axial force of the $j$th fastening rod with a crack can be expressed as:
The potential energy of $j$th cracked fastening rod can be given as:
Substituting the Eqs. (1) and (5) into the Eq. (11), the total potential energy of $j$th cracked fastening rod and the others with no crack can be given as:
with:
$p=EAf\left(\lambda \right){r}^{2}\cdot \frac{\mathrm{s}\mathrm{i}\mathrm{n}\left[2\left(\omega t+{\gamma}_{i}\right)\right]}{\pi {L}_{0}},\mathrm{}\mathrm{}\mathrm{}\mathrm{}\mathrm{}f\left(\lambda \right)=\left(\alpha +\mathrm{s}\mathrm{i}\mathrm{n}\alpha \lambda \mathrm{s}\mathrm{i}\mathrm{n}\alpha \right),$
and the addon stiffness matrix stiffness matrix ${\mathbf{K}}_{rodc}$ as followed in Eq. (13):
It can be found that Eq. (5) and Eq. (12) are different, which shows the cracked rodfastening rotor system will introduce the addon stiffness matrix ${\mathbf{K}}_{rodc}$ as shown in Eq. (13) besides ${\mathbf{K}}_{rod}$ in Eq. (6) compared with intact rodfastening rotor system.
It is note that the additional stiffness matrix of the cracked fastening rod as shown in Eq. (13) is asymmetric. This asymmetry will break the existed relatively steady state of rotor system resulting in the change of the system stability. Meanwhile, the contribution of the additional stiffness matrix introduced by the crack is to reduce total stiffness of the system.
2.3. Dynamic equations of cracked rotor bearing system
The finite element method with Timoshenko beam element with four degrees of freedoms at each node is employed to discretize the rotor into 11 elements [2427]. The four disks, fastening rods and two radial cylindrical bearings are assembled together with the rotor through the finite element method. Then the dynamic equation of the cracked rodfastening rotor bearing system is formulated as follows:
with:
${\mathbf{Q}}^{S}={\mathbf{Q}}^{r}+{\mathbf{Q}}^{d},{\mathbf{F}}^{S}={\mathbf{F}}_{rod}+{\mathbf{F}}_{oil},$
where $\mathbf{M}$, $\mathbf{G}$, $\mathbf{K}$, and $\mathbf{Q}$ are the mass matrix, gyroscope matrix, stiffness matrix and the external force vector (including gravity and unbalance force), respectively, and the corresponding superscript ‘$S$’, ‘$r$’, and ‘$d$’ stand for the whole system, rotor shaft and disk, respectively. $\mathbf{x}$ is one single node displacement vector, which have translational and rotational displacement about $X$and $Y$axes of the fixed coordinate system, i. e. $\mathbf{x}={[x,y,\psi ,\phi ]}^{T}$. So for the displacement vector of a rotor with $n$ nodes, it can be given as ${\mathbf{x}}^{\mathrm{S}}={\left[{x}_{1},{y}_{1},{\psi}_{1},{\varphi}_{1},\cdot \cdot \cdot ,{x}_{n},{y}_{n},{\psi}_{n},{\varphi}_{n}\right]}^{T}$. ${\mathbf{K}}_{rod}^{S}$ is the $4n\times 4n$ (node number $n=$ 12) stiffness matrix which consists of ${\mathbf{K}}_{rod}$. ${\mathbf{K}}_{rodc}^{S}$ is the $4n\times 4n$ stiffness matrix of which the entries of zero entries except at the crack node location are equal to ${\mathbf{K}}_{rodc}$. ${\mathbf{F}}_{rod}$ and ${\mathbf{F}}_{oil}$ are $4n\times 1$ matrix of which the entries of zero entries except at the corresponding node location are equal to ${\mathbf{f}}_{rod}$ and ${\mathbf{f}}_{oil}$, respectively. The oil force vector can be expressed as ${\mathbf{f}}_{oil}=({f}_{bx},\mathrm{}{f}_{bx},\mathrm{}0,\mathrm{}0{)}^{T}$ , which can be obtained from the typical infinite long bearings assumption [28].
3. Method of solution and nonlinear analysis
3.1. Method of solutions
The whole system have 48 DOFs which contain linear and nonlinear DOFs. Although it is not very high dimension for advanced computer technology nowadays, it also need consume much time for real time simulation at different speeds. To save the computing time and retain necessary DOFs information, the free interface modal synthesis technology [22, 23 29, 30] are employed to reduce the system DOFs. The nonlinear DOFs corresponding to two bearing nodes and four disks nodes and other two corresponding nodes of linear DOFs are retained. Then the reduced system can be given as follows:
where $\mathbf{M}={\mathbf{T}}^{T}{\mathbf{M}}^{S}\mathbf{T}$, $\mathbf{G}={\mathbf{T}}^{T}{\mathbf{G}}^{S}\mathbf{T}$, $\mathbf{K}={\mathbf{T}}^{T}{\mathbf{K}}^{S}\mathbf{T}$, and $\mathbf{Q}={\mathbf{T}}^{T}{\mathbf{Q}}^{S}+{\mathbf{T}}^{T}{\mathbf{F}}^{S}$. $\mathbf{q}$ is the reduced displacement vector. $T$ is a transformation matrix being introduced to reduce the original system. By introducing the state variable $\mathbf{X}={\left({\mathbf{q}}^{T},\mathrm{}{\dot{\mathbf{q}}}^{T}\right)}^{T}$, the corresponding reduced system equations in a state space can be written as follows:
By system reduction, the local nonlinearity of nodes which locates in bearings and disks are retained as well as other two linear nodes, which means 32 DOFs in total are kept. Then the nonlinear stability and bifurcation behaviors can be obtained by numerical simulations.
Assuming that the system is subjected to the external periodic load ${\mathbf{Q}}_{ex}\left(t\right)$ with period ${T}_{0}$, i.e. ${\mathbf{Q}}_{ex}\left(t\right)={\mathbf{Q}}_{ex}(t+{T}_{0})$, which originates from the mass eccentricity. Then periodic solutions can be are calculated by solving a two point boundary value problem, which is defined by Eq. (19) supplemented with the boundary condition $\mathbf{X}\left(t\right)=\mathbf{X}(t+{T}_{0})$. It can be written as:
with $\mathbf{f}(\mathbf{X},\mathrm{}t,\mathrm{}\lambda )=\left(\begin{array}{c}\dot{\mathbf{q}}\\ {\mathbf{M}}^{1}\left(\mathbf{Q}\mathbf{K}\mathbf{q}\mathbf{G}\dot{\mathbf{q}}\right)\end{array}\right)$, where $\lambda $ is a system parameter, which can be the angular speed $\omega $ or the mass eccentricity $e$, etc.
The periodic solutions of the system will become unstable in certain intervals of system parameters. It is important to determine the unstable intervals and which kind of nonlinear dynamic behaviors of system among the periodic, quasiperiodic, and chaotic it is. Here, for a given system parameter, the shooting method [22, 23, 29, 3133] is adopted to obtain the details of periodic solutions. Then the pathfollowing technique [31, 33] is used to investigate how a periodic solution is influenced by a change of $\lambda $. The whole solution braches of system can be found with this combined technique, which is consist of a predictorcorrector mechanism as shown in Eq. (21) in nature:
For the Eq. (21), the next step solution, i.e. ${\mathbf{X}}_{n+1}$ at ${\lambda =\lambda}_{n+1}$, can be determined by starting from a known solution ${\mathbf{X}}_{n}$ at ${\lambda =\lambda}_{n}$, and combining with the corrected mechanism by using shooting method.
Lastly, the Floquet theory [22, 33] is employed to determine the local stability of periodic motion of nonlinear system. The procedure involves calculating the largest eigenvalues (Floquet multipliers) of the Jacobian matrix (the details see the [22, 23]) produced in the process of the shooting method. In general, the Floquet multipliers must be within the unit circle in the complex plane. While with the change of the system parameter, the stable periodic solution of system will happen to lose stability, which will show different forms of bifurcation.
According to the situation of the maximum Floquet multipliers through the unit circle in the complex plane, the forms of bifurcation can be classified into three modes i.e. perioddoubling bifurcation, quasiperiodic bifurcation and “cyclefol” or “transcritical” bifurcation [23].
Each finite element node of system as shown in Fig. 1 is marked by integer from 1 to 12 in sequence. The corresponding parameters of the cracked and intact rodfastening rotor bearing system are given in Table 1. The mass eccentricities of four disks are represented by ${e}_{a}$, ${e}_{b}$, ${e}_{c}$, and ${e}_{d}$ (${e}_{a}={e}_{b}={e}_{c}={e}_{d}=e$) which results in the unbalance forces of system. Meanwhile, the numerical results of rodfastening rotor system model with no crack as referred in [22, 23] are also given for comparison. The simulation results are obtained as shown from Fig. 311, respectively, through Fortran program by changing corresponding parameters.
3.2. Simulation results and nonlinear analysis
3.2.1. Effects of crack on the system stability and bifurcation
For a given crack depth $h=$ 0.1${r}_{0}$ of the cracked fastening rod, the regulations of the stable and unstable solutions of the system with the change of the system parameters $e$ and $\omega $ for both cracked rodfastening rotor bearing system and intact ones are shown in Fig. 3(a).
Fig. 3. a) $e$$\omega $ curves of the solution set of stability and bifurcation transition of the cracked and intact rotor systems, b) effects of the crack depth on the system stability and bifurcation
a)
b)
Compared with intact rodfastening rotor system, in general, the stability and instability regions of the cracked ones also have three parts, the stable $T$ periodic motion region ${S}_{T}$, the perioddoubling motion region S_{D} and the quasiperiodic motion region ${S}_{Q}$ which are developed by the corresponding two borderlines of TDline, TQline and QDline, respectively, as shown in Fig. 3(a). The TDline and TQline are the perioddoubling bifurcation borderline and quasiperiodic bifurcation borderline, respectively. Periodicdoubling motion or quasiperiodic bifurcation motion will occur when the rotating speed ω or the mass eccentricities $e$ crosses TDline or TQline. The dashed QDline is the critical parting line of perioddoubling bifurcation motion region S_{T} and quasiperiodic bifurcation motion region S_{Q}. The symbols ${w}_{b0}$ and ${w}_{b1}$ in Fig. 3(a) as well as ${w}_{b2}$ and ${w}_{b3}$ mentioned later in text are linear critical speed of the equilibrium point for the balanced rodfastening rotor system ($e=$ 0) and ${w}_{b0}$, ${w}_{b1}$, ${w}_{b2}$ and ${w}_{b3}$ correspond to the crack depth equaling to 0, 0.1${r}_{0}$, 0.2${r}_{0}$, and 0.3${r}_{0}$, respectively. Hopf bifurcation will occur for the system and subsequently lose stability when the rotating speed exceeds linear critical speed for the balanced rodfastening rotor system.
It is worth noting that there are some different details between cracked rodfastening rotor system with a transverse open crack in a fastening rod and intact ones as follows
Firstly, the $e$$w$ curve of cracked rotor system tends to move to the lower right as a whole and the QDline tends to a downward move. These differences are mainly caused by the existence of crack of the fastening rod which will introduce the additional stiffness and cause system stiffness to reduce. While these changes are very small when the rotating speed is approximately on the left side of the first saddleback of TDline which corresponds to the location of the first resonance peak in Fig. 4(a) probably. This means the influences of shallow crack of the fastening rod on system dynamic behaviours is small for rodfastening rotor system when they work under the rotating speeds corresponding to the first resonance peak.
Fig. 4. Vibration amplitudes when $h=$ 0.1${r}_{0}$ and $e=$ 1 μm: a) bearing node, b) middle disk node
a)
b)
Secondly, it can be found that it happens to two saddlebacks of TDline as shown in Fig. 1 which approximately corresponds to the two resonant peaks of bearing node for cracked rodfastening rotor system as shown in Fig. 4(a). In contrast with the intact rotor system, the TQline shows just a saddleback. Thus, they will perform different dynamic behavious and stability in the location of second saddleback of cracked rodfastening rotor system which one is stable and another is periodicdoubling bifurcation behaviours because of the presence of crack on the surface of the fastening rod. It is also worthwhile to note that the vibration amplitudes of the cracked rodfastening rotor system under stable region with 1 μm mass eccentricity is bigger compared with the intact rotor system as shown in Fig. 4(a, b), especially for the middle disk node as shown in Fig. 4(b).
Thirdly, the TQline shows a linear growth trend with the increment of rotating speeds and the mass eccentricities for two systems. Although the most part of TQline seems to move slightly to the right for cracked rotor system, it tends to move slightly to the left when the mass eccentricities equals to zero or near the zero regions. It can be seen that the linear critical speed ${w}_{b1}$ of cracked rotor system locates on the right of the linear critical speed ${w}_{b0}$ of intact ones. This shows the cracked rodfastening rotor system will early to lose stability for balanced ones (mass eccentricities $e=$ 0) or very small mass eccentricities compared with intact rotor system.
3.2.2. Effects of crack depth on the system stability and bifurcation
From the Fig. 3(b), It can be found the effects of crack depth on the system stability and bifurcation. With the increment of crack depth, the TDline, QDline and TQline happen to move down except the part between the two saddlebacks which increases. These shows the system stability gradually decreases on the whole due to the reduction of the system stiffness resulting from the crack of the fastening rod. It is note that the influence of crack becomes obvious with the increment of crack depth when the rotating speed locates on the left side of the first downfold of the TDline, especially for the crack depth greater than 0.2${r}_{0}$. The rotor system begins to become periodicdoubling motion even the mass eccentricities equal to zero when the crack depth comes up to 0.3${r}_{0}$. For the balanced rodfastening rotor system ($e=$ 0), the linear critical speed happens to a little shift to left with the increment of crack depth such as ${w}_{b3}$ on the left of ${w}_{b2}$ and ${w}_{b2}$ on the left of ${w}_{b1}$. This reveals the stability of the balanced rodfastening rotor system will decrease with the increment of crack depth which performs some differences on linear critical speed. Besides, it is worth note that the periodicdoubling motion occurring under small or zero mass eccentricities condition is the characteristic signal of cracked rodfastening rotor system, which always performs stable $T$ periodic motion in corresponding region for intact rodfastening rotor system. These may be useful for detecting the presence of a crack and its depth for this kind of rodfastening rotor system
3.2.3. Effects of mass eccentricity
In this part, the effects of typical mass eccentricities $e=$ 0 μm, 8.3 μm, and 12 μm on the dynamic behaviours such as orbits of periodic motion, vibration model, frequency spectrums analysis, and Poincare map are studied as well as the intact ones in literature for comparison.
(1) Mass eccentricity $e=$ 0 μm.
It can be obtained that the cracked rodfastening rotor system and intact ones lose their stabilities at ${w}_{b1}$ (12150 rpm) and ${w}_{b0}$ (12160 rpm), respectively from Fig. 3(a). While the form of transition from steady state to full unstable state is different. After crossing the linear critical speed ${w}_{b1}$ and ${w}_{b0}$, for example at 12240 rpm, the cracked rotor system loses stability by quasiperiodic bifurcation as shown in Fig. 5(a) which shows the orbits of whole 12 nodes and the intact ones by Hopf $T$ periodic solution as shown in Fig. 5(b). The vibration modes of rotor shaft of two systems at a transient time is different and it shows the vibration amplitude of cracked rotor system tends to be larger than the intact ones due to the presence of the crack of rodfastening as depicted in Fig. 5(c).
Fig. 5. Periodic solutions for all nodes when $e=$ 0 μm and $w=$ 12240 rpm: a) Quasiperiodic solutions for cracked rodfastening rotor system with $h=$ 0.1${r}_{0}$, b) Hopf $T$ periodic solutions for intact systems, c) comparison of the whole vibration modes of two systems
a)
b)
c)
In order to further explore the dynamic behaviours, Fig. 6(a), (b) and (c) shows the orbits and frequency spectrum of bearing node. It can be seen clearly that the quasiperiodic bifurcation behaviours for cracked systems and Hopf $T$ periodic bifurcation for intact ones in Fig. 6(a). Besides there are some differences in frequency component, which occurs to whirling frequency about 204 Hz for cracked system except the whirling frequency about 120 Hz compared with the intact ones as shown in Fig. 6(b, c).
(2) Mass eccentricity $e=$ 8.3 μm.
According to the Fig. 3(a), it can be known that the cracked rodfastening rotor system occurs to lose stability at $w=$ 13450 rpm when mass eccentricity $e=$ 8.3 μm as well as at $w=$ 13370 rpm for intact ones. Fig. 7(a) shows the periodicdoubling motion at $w=$ 13458 rpm and periodicdoubling motion at $w=$ 13440 rpm of bearing node for two systems respectively when $e=$ 8.3 μm. Poincare maps is a closed curve consisted of limited points for cracked system and the others are two isolated points for intact ones in Fig. 7(b), which confirms the corresponding motions are periodicdoubling and periodicdoubling, respectively. The frequency spectrums of $Y$ direction are illustrated in Fig. 7(c) which shows the frequency components are very consistent. This means that it is difficult to distinguish the cracked and intact rodfastening rotor bearing systems by frequency components on this condition.
Fig. 6. The bearing node dynamic behaviours when $e=$ 0 μm and $w=$ 12240 rpm for two systems: a) orbits, b) and c) frequency spectrums of $X$ and $Y$ direction, respectively
a)
b)
c)
Fig. 7. Periodicdoubling ($w=$ 13458 rpm) and quasiperiodic ($w=$ 13440 rpm) solution of bearing nodes for two systems respectively when $e=$ 8.3 μm: a) orbits, b) Poincare map, c) frequency spectrums
a)
b)
c)
Fig. 8. Solutions for all nodes when $e=$ 8.3 μm: a) periodicdoubling solution ($w=$ 13458 rpm) for cracked rodfastening rotor system, b) quasiperiodic solution ($w=$ 13440 rpm) for intact ones, c) comparison of the whole vibration modes for two systems
a)
b)
c)
Fig. 8(a, b) shows the periodicdoubling motion and quasiperiodic motion of the whole nodes for cracked and intact rodfastening rotor system, respectively. Fig. 8(c) gives the vibration modes of two systems. Because of the presence of crack for cracked system, the vibration amplitude of cracked system is larger than the intact ones.
(3) Mass eccentricity $e=$ 12 μm.
The nonlinear dynamic behaviours for two systems are very consistent when the crack depth is 0.1${r}_{0}$ and the system work on the left side of the first saddleback according to $e$$w$ diagram in Fig. 3(a). It can be seen that the periodic motions of bearing nodes occur for cracked and intact rotor system as shown in Fig. 9(a), and the two isolated points of Poincare maps as shown in Fig. 9(b) also confirm this nonlinear dynamic behaviours. Besides the frequency components of bearing node of frequency spectrums of $X$ direction in Fig. 9(c) are also same. In addition, the solutions of whole nodes are very consistent and periodic motions as shown in Fig. 10(a) and (b) as well as the vibration modes in Fig. 10(c). This reveals that the effects of crack are very small to some extent, especially when the system works under in the range of the first resonance peak and has a slight crack depth. While this phenomenon will change with the increment of crack depth as shown in Fig. 3(b).
Fig. 9. Periodicdoubling solution ($w=$ 6400 rpm) of bearing nodes for two systems respectively when $e=$ 12 μm: a) orbits, b) Poincare map, c) frequency spectrums of $X$ direction
a)
b)
c)
Fig. 10. Periodicdoubling solutions for all nodes when $e=$ 12 μm and $w=$ 6400 rpm: a) cracked rodfastening rotor system, b) intact rotor system, c) the whole vibration modes for two systems
a)
b)
c)
4. Conclusions
A transverse open crack model of a fastening rod is developed, the nonlinear dynamic model of rodfastening rotor bearing system with crack on the surface of a fastening rod is established based on the finite element method and the stability and bifurcation of system as well as the effects of crack depth and the mass eccentricities on system are investigated. By numerical simulations and nonlinear analysis, some special characteristics of cracked rodfastening rotor system are founded compared with the intact rodfastening rotor system in the literature. It also explains the validity of proposed model. The main conclusions are developed as follows:
1) In general, the stability will reduce, and the vibration amplitudes will increase in steady state when there is a crack on the surface of the fastening rod. Because of the presence of crack, this can introduce the addon stiffness resulting in the reduction of system stiffness and the asymmetric effect. Meanwhile, it will happen to two saddlebacks of periodicdoubling border lines in $e$$w$ diagram which corresponds to the two resonant peaks of bearing node in ${A}_{x}$$w$ diagram. The change of the solution sets of stability and bifurcation transition with the mass eccentricity and rotating speed become complicated when there is a crack compared with the intact system. The influences of the presence of crack on the nonlinear dynamic of system are not obvious when the crack depth is small and the rotating speed is on the left side of the first saddleback of periodicdoubling borderline.
2) With the increment of the crack depth, the reduction of system stiffness and the asymmetric effect become more obvious. This causes the system instability to become more severe and complicated. The borderlines among the stability, periodicdoubling bifurcation, and quasiperiodic bifurcation regions occur to decline except the parts between the first and second saddleback.
For the balanced rodfastening rotor system ($e=$ 0 or near zero), the linear critical speed decreases with the increment of crack depth and the cracked system loses stability by quasiperiodic bifurcation while the intact system by Hopf $T$ periodic bifurcation instead. Besides, the periodicdoubling bifurcation easily arises with increment of crack depth when the rotor system works under the balanced or small mass eccentricities states compared with the intact systems in which always represents a stable status.
3) The results of numerical simulation indicate that the effects of crack on the system play a dominant position when the mass eccentricity is zero or small and there exist some differences in orbits, Poincare map, frequency component, and the vibration modes. These provide some useful special characteristics for detecting the presence of crack especially in orbits and frequency components. With the increment of the mass eccentricity and when it exceeds a critical value, the effects of mass eccentricity will play a dominant position and it is not easy to distinguish the two systems just from the routine orbits and frequency components in this state.
Acknowledgements
This research project was supported by the National Natural Science Foundation of China under Grant No. 51475357 and No. 51705399.
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Cited By
Archive of Applied Mechanics
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2021

Archive of Applied Mechanics
Longkai Wang, Ailun Wang, Miao Jin, Qike Huang, Yijun Yin

2020
