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International Journal of Research in Engineering and Science (IJRES)
ISSN (Online): 2320-9364, ISSN (Print): 2320-9356
www.ijres.org Volume 3 Issue 11 ǁ November. 2015 ǁ PP.12-17
www.ijres.org 12 | Page
Study on Vibration Reduction Effect of the Rail Vehicle with Axle
Dynamic Vibration Absorber
LI Qiong, WEN Yong-peng*
, ZHOU Wei-hao, XU Xiao-jun
(College of Urban Railway Transportation, Shanghai University of Engineering Science, China)
ABSTRACT: To reduce the vertical vibration of the vehicle, the vehicle model including the axle dynamic
vibration absorber is established, and the vertical vibration acceleration spectrum of the wheel, the steering
frame and the body is obtained by numerical simulation. The vibration reduction effect of the dynamic vibration
absorber is analyzed. The results show that the axle dynamic vibration absorber not only has a good vibration
reduction effect on the wheel, but also has an important effect on the vertical vibration of the bogie and the
vehicle body.
Keywords: Dynamic vibration absorber, Axle, Vertical vibration, Mass ratio, Damping
I. INTRODUCTION
The vibration of rail vehicle may cause wheel, bogie and other components cracks and other damages,
which may affect the safe operation of the vehicle. V The wheel-rail interaction leads to vehicle vibration and
passes primary and second suspension system to the bogie and the car body. Therefore, the research on vehicle
vibration damping device is very necessary.
At present, many scholars have studied the vehicle model, Zhai Wan-ming[1] established a vehicle/track
coupled mode. The vehicle was simplified as a multi-degree of freedom model, the track is considered as
a Timoshenko beam, Vehicle and track model are considered more complete; Zhao Honglun [2] established a
finite element model of vehicle systems for analysis, and provided a reference for the development of rail
vehicles. In addition, in order to reduce the vertical vibration of the vehicle, many scholars have established a
vehicle model with dynamic vibration absorber, Foo [3] proposed a dynamic vibration absorber which is
installed at the bottom of the car body, The results show that vibration can be reduced in some parts of the
vehicle body; Zeng Jing [4] established the vehicle model installation dynamic vibration absorber and
analysis its damping, The research results show that the damping performance of the vibration absorbers is very
good in the low frequency and at speed greater than 150km/h; Zhou Jingsong [5-6]established the
vehicle model with dynamic vibration absorber, and introduced the vehicle running stability index to discuss the
damping performance of vehicle dynamic vibration absorber, obtain that dynamic vibration absorber can
make the running stability of vehicles reached excellent, and the higher its quality the better its damping
performance; Tomioka [7]considered the bogie as a dynamic vibration absorber. The research results show that
it can significantly reduce the bending vibration of car body. In general, the vehicle model is becoming more
and more complex, and the results are more realistic. Moreover, the dynamic vibration absorber is seemed as a
an effective device for vehicle vibration reduction.
Therefore, according to Lagrange equation, in order to reduce the vertical vibration of the vehicle, we
establish vehicle dynamics model with an axle dynamic vibration absorber, in which the dynamic vibration
absorber mounted on the axle portion of the system by reducing wheel vibration throughout the vehicle to
reduce the effect of vibration. According to the obtained vehicle acceleration power spectral density of the
components, vehicle dynamic vibration absorber damping effect is analysis carefully.
II. WHEEL MODEL
The dynamic vibration absorber is mounted on the axle, as shown in Fig. 1, the axle wrap a layer of shock-
absorbing materials and vibration absorber simplified model to simplify mass, spring and damping is shown in
Fig. 2. Model has a body of ups and downs and nod (two degrees of freedom), front and rear bogies of ups and
downs and nod (four degrees of freedom), four wheels drifting (four degrees of freedom) and dynamic vibration
absorber ups and downs (one degree of freedom) simplified model fourteen degrees of freedom.
*Corresponding author
E-mail address: yp_wen@163.com
Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber
www.ijres.org 13 | Page
Fig.1 Wheel of dynamic vibration absorber schematic
Fig.2 Vehicle model including the dynamic vibration absorber of a wheel
In Fig. 2, the vertical displacement of the vehicle to the right, , cZ 、 1tZ 、 2tZ respectively body, front and
rear bogie vertical displacement, c 、 1t 、 2t respectively front and rear bogie nod corner, 1wZ 、 2wZ 、 3wZ 、
4wZ respectively for the first one, two, three and four of the vertical displacement.
According to Lagrange equation for vehicle dynamics model is derived and its kinetic equation written in
compact form as follows:
          M Z C Z K Z F    , (1)
In the formula:  Z is the displacement matrix,  M is the mass matrix,  K is the stiffness matrix,  C is the
damping matrix,  F is the force matrix for the wheel. In the matrix Z , 1dZ 、 2dZ 、 3dZ 、 4dZ are the vertical
displacement of the dynamic vibration absorber corresponding to the corresponding wheel is represented.
       = r FF C q K q , (2)
 
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
r
r
r
r
r
C
C
C
C
C
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0
0 0 0
0 0 0
0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
0 0 0 0
r
r
r
r
r
K
K
K
K
K
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
 
, (3)
Dynamic vibration absorber
Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber
www.ijres.org 14 | Page
III. MODEL SOLVING
The Fourier transform (1) is performed in the frequency domain:
          
12
H M j C K F  

      , (4)
Since the excitation of each wheel has a certain delay, the input of the three wheel is considered as the input of
the first wheel.
Wheels by incentive matrix:
   1 2 3 4 1( ) ( ) ( ) ( ) ( )
T
q q q q Q q     , (5)
In the formula: 1 ( )q  、 2 ( )q  、 3 ( )q  、 4 ( )q  respectively, the excitation of the four wheels in the frequency
domain.
Including:
  32 4
= 1
Tj Tj T j T
Q e e e  
   , (6)
In the formula 2 2 tT l u , 3 2 cT l u ,  4 2 t cT l l u  .
It can be obtained that the frequency response matrix of each part of the vehicle is not smooth, and each element
of the matrix is the frequency response function of the displacement of the vehicle.
         1 14=
T
h H Q h h              , (7)
According to the frequency response function of the displacement, the acceleration response function can be
obtained.
 
 
 
 1
2 2
1
i
i
iZ q
Z
h h
q

   

    , (8)
     1 1
2
1i i
Z q Z q
G h q   
  , (9)
In the formula:   1iZ q
h   is the acceleration frequency response function of the corresponding component
relative to the irregularity excitation is expressed,   1iZ q
G   is the acceleration power spectral density of the
corresponding components for the irregularity excitation is indicated.
Although the acceleration power spectral density can be very convenient to analyze the frequency characteristics
of vertical vibration of vehicle system, the acceleration of vertical vibration of the vehicle in the frequency range
of 1 to n frequency range is required:
   1
1
2n
ii zG G d


  
   
, (10)
IV. SIMULATION RESULTS
4.1 MODEL PARAMETERS
Based on one type of vehicle as an example, According to the dynamic vibration absorber principle
can determine the dynamic vibration absorber absorbing quality and stiffness, the parameters are shown in Table
1, With American class six track irregularity spectrum as incentive of the vehicle vertical vibration model.
Table1 A certain type of vehicle parameters and track parameters
Meaning Parameter symbol Value
Mass of vehicle Mb/kg 4.18×104
Car body pitch inertia Jb/(kg·m2) 1.686×106
Mass of bogie Mt/kg 2.8×103
Bogie pitch inertia Jt/( kg·m2) 1.93×103
Secondary spring stiffness per bigie Ks2/( kN·m-1) 6×105
Secondary damping per bogie Cs2/( kN·s·m-1) 1.1×104
Primary spring stiffness per axle Ks1/( kN·m-1) 1.11×106
Primary spring damping per axle Cs1/( kN·s·m-1) 2.4×104
Half of bogie centers lb/m 9
Half of bogie wheel base lw/m 1.25
Mass of Dynamic vibration absorber Md/kg 140
Dynamic vibration absorber stiffness Kd/( kN·m-1) 4×105
Dynamic vibration absorber damping Cd/( kN·s·m-1) 50
Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber
www.ijres.org 15 | Page
4.2 PERFORMANCE ANALYSIS OF DYNAMIC VIBRATION ABSORBER
To simulate the model and obtain the components of the vehicle vertical vibration acceleration power
spectral density.
Fig.3 Effect of dynamic vibration absorber on the vibration of wheel set
The wheel vertical acceleration power spectral density curves of vibration is as shown in Fig. 3, It can be
seen from Fig. 3 that the wheel's vertical vibration at 40Hz with excitation frequency resonance and reached
peak. Therefore, the wheel vibration is most intense, resulting in damage to the wheel strength, seriously
affecting the safe operation of the vehicle. After installing the dynamic vibration absorber, vertical vibration of
the wheel has been significantly reduced in the resonance frequency.
Wheel vertical vibration is passed primary suspension up to the bogie, The wheel vibration directly affects
the vibration situation of the bogie, the Front and rear bogie vertical acceleration power spectral density curves
of vibration is as shown in Figure 4, It can be seen from Fig. 4 thatdue to the wheels produce resonance in 40Hz,
leading to the bogie at 40Hz also produces vibration peak, dynamic vibration absorber reduce the vertical
vibration of wheel at the resonant frequency, Vertical vibration transmitted to the bogie has been weakened,
Therefore, the axle dynamic vibration absorber can not only reduce the wheel vertical vibration can also weaken
the vertical vibration of the bogie.
(a) Front bogie
PSDofFrontbogie/m2s-3
f /Hz
f /Hz
PSDofWheelset/m2s-3 No DVA
With DVA
Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber
www.ijres.org 16 | Page
(a) Rear bogie
Fig.4 The influence of dynamic vibration absorber on the vibration of bogie
The car body vertical acceleration power spectral density curves of vibration is as shown in Fig. 5, It can be
seen from Fig.5 that due to bogie vertical vibration in the vicinity of 40Hz is weakened, so the vertical vibration
of the vehicle body vibration at this frequency is also weakened. However, the body's natural frequency of about
1.5Hz, body vertical vibration of the energy is concentrated at low frequencies near the natural frequency. The
vibration energy is smaller in the near of 40Hz frequency. Therefore, although the dynamic vibration absorber
can reduce vibration here, the effect of reduce the vehicle's vertical vibration is limited
Fig.5 Effect of dynamic vibration absorber on the vibration of car body
The wheel has a good vertical vibration damping effect on the wheel. In order to improve the vibration
performance, the mass ratio of the dynamic vibration absorber is improved. Fig. 6 shows the influence of the
mass ratio of the dynamic vibration absorber on the vibration absorption performance of the dynamic absorber.
The mass ratio of the dynamic vibration absorber can obviously improve the vibration reduction performance.
Moreover, the vibration frequency band of the dynamic vibration absorber is gradually widened.
PSDofCarbody/m2s-3
f /Hz
PSDofRearbogie/m2s-3
f /Hz
Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber
www.ijres.org 17 | Page
Fig.6 Influence of mass ratio on the vibration reduction effect of dynamic vibration absorber
V. CONCLUSIONS
Axle vibration absorber for vertical vibration of the wheel not only has a good inhibition, but also on the
bogie and the body has a important damping effect. For the vertical vibration of the vehicle body is mainly
concentrated in the low frequencies, therefore, the axle dynamic vibration damping effect on the body is limited.
The vibration reduction effect can be improved by increasing the mass ratio of the axle dynamic vibration
absorber. The vibration of the wheel is radiated from the outside; therefore, the vibration of the axle can be
controlled by reducing the vertical vibration of the wheel.
VI. ACKNOWLEDGEMENTS
The authors would like to acknowledge the support of National Natural Science Foundation of China (Grant
No. 11472176), Natural Science Foundation of Shanghai (Grant No. 15ZR1419200) and Discipline
Construction Project for Transportation Engineering (Grant No. 13SC002).
REFERENCES
[1] XU Zhisheng ZHAI Wanming Prediction and Control of Wheel/Rail Noise for Rail Transit [J].China Railway Science,
2006,27(1):138-139.
[2] ZHAO Hong-lun YU Cheng-liang WANG Wen-bin. Study on Optimization Design of Carbody Structure of High-speed Maglev
Train [J]. Journal of the China Railway Society, 2007,04:43-47.
[3] FOO E,GOODALL R M.Active Suspension Control of Flexible-Bodied Railway Vehicle Using Electro-Hydraulic and
Electromagnetic Actuators[J].Control Engineering Practice,2000,8:507-518.
[4] ZENG Jing;WU Ping-bo;HAO Jian-hua.Analysis of Vertical Vibration Reduction for Railway Vehicle Systems [J]. China
Railway Science, 2006,27(3):62-67.
[5] ZHOU Jinsong ZHANG Wei SUN Wenjing .Vibration Reduction Analysis of the Dynamic Vibration Absorber on the Flexible
Carbody of Railway Vehicles[J]. China Railway Science,2009,30(3):86-90.
[6] ZHOU Jinsong GONG Dao REN Lihui.Simulation on Passive Vibration Control of Flexible Carbody of Railway Passenger
Vehicles[J]. Journal of TongJi University (Natural Science),2009,37(8):1085-1089.
[7] Takahiro Tomioka, Tadao Takigami. Reduction of bending vibration in railway vehicle carbodies using carbody–bogie dynamic
interaction[J]. Vehicle System Dynamics.2010.4.467-486.
No DVA
μ=0.003
μ=0.015
f /Hz
PSDofWheelset/m2s-3

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Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber

  • 1. International Journal of Research in Engineering and Science (IJRES) ISSN (Online): 2320-9364, ISSN (Print): 2320-9356 www.ijres.org Volume 3 Issue 11 ǁ November. 2015 ǁ PP.12-17 www.ijres.org 12 | Page Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber LI Qiong, WEN Yong-peng* , ZHOU Wei-hao, XU Xiao-jun (College of Urban Railway Transportation, Shanghai University of Engineering Science, China) ABSTRACT: To reduce the vertical vibration of the vehicle, the vehicle model including the axle dynamic vibration absorber is established, and the vertical vibration acceleration spectrum of the wheel, the steering frame and the body is obtained by numerical simulation. The vibration reduction effect of the dynamic vibration absorber is analyzed. The results show that the axle dynamic vibration absorber not only has a good vibration reduction effect on the wheel, but also has an important effect on the vertical vibration of the bogie and the vehicle body. Keywords: Dynamic vibration absorber, Axle, Vertical vibration, Mass ratio, Damping I. INTRODUCTION The vibration of rail vehicle may cause wheel, bogie and other components cracks and other damages, which may affect the safe operation of the vehicle. V The wheel-rail interaction leads to vehicle vibration and passes primary and second suspension system to the bogie and the car body. Therefore, the research on vehicle vibration damping device is very necessary. At present, many scholars have studied the vehicle model, Zhai Wan-ming[1] established a vehicle/track coupled mode. The vehicle was simplified as a multi-degree of freedom model, the track is considered as a Timoshenko beam, Vehicle and track model are considered more complete; Zhao Honglun [2] established a finite element model of vehicle systems for analysis, and provided a reference for the development of rail vehicles. In addition, in order to reduce the vertical vibration of the vehicle, many scholars have established a vehicle model with dynamic vibration absorber, Foo [3] proposed a dynamic vibration absorber which is installed at the bottom of the car body, The results show that vibration can be reduced in some parts of the vehicle body; Zeng Jing [4] established the vehicle model installation dynamic vibration absorber and analysis its damping, The research results show that the damping performance of the vibration absorbers is very good in the low frequency and at speed greater than 150km/h; Zhou Jingsong [5-6]established the vehicle model with dynamic vibration absorber, and introduced the vehicle running stability index to discuss the damping performance of vehicle dynamic vibration absorber, obtain that dynamic vibration absorber can make the running stability of vehicles reached excellent, and the higher its quality the better its damping performance; Tomioka [7]considered the bogie as a dynamic vibration absorber. The research results show that it can significantly reduce the bending vibration of car body. In general, the vehicle model is becoming more and more complex, and the results are more realistic. Moreover, the dynamic vibration absorber is seemed as a an effective device for vehicle vibration reduction. Therefore, according to Lagrange equation, in order to reduce the vertical vibration of the vehicle, we establish vehicle dynamics model with an axle dynamic vibration absorber, in which the dynamic vibration absorber mounted on the axle portion of the system by reducing wheel vibration throughout the vehicle to reduce the effect of vibration. According to the obtained vehicle acceleration power spectral density of the components, vehicle dynamic vibration absorber damping effect is analysis carefully. II. WHEEL MODEL The dynamic vibration absorber is mounted on the axle, as shown in Fig. 1, the axle wrap a layer of shock- absorbing materials and vibration absorber simplified model to simplify mass, spring and damping is shown in Fig. 2. Model has a body of ups and downs and nod (two degrees of freedom), front and rear bogies of ups and downs and nod (four degrees of freedom), four wheels drifting (four degrees of freedom) and dynamic vibration absorber ups and downs (one degree of freedom) simplified model fourteen degrees of freedom. *Corresponding author E-mail address: yp_wen@163.com
  • 2. Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber www.ijres.org 13 | Page Fig.1 Wheel of dynamic vibration absorber schematic Fig.2 Vehicle model including the dynamic vibration absorber of a wheel In Fig. 2, the vertical displacement of the vehicle to the right, , cZ 、 1tZ 、 2tZ respectively body, front and rear bogie vertical displacement, c 、 1t 、 2t respectively front and rear bogie nod corner, 1wZ 、 2wZ 、 3wZ 、 4wZ respectively for the first one, two, three and four of the vertical displacement. According to Lagrange equation for vehicle dynamics model is derived and its kinetic equation written in compact form as follows:           M Z C Z K Z F    , (1) In the formula:  Z is the displacement matrix,  M is the mass matrix,  K is the stiffness matrix,  C is the damping matrix,  F is the force matrix for the wheel. In the matrix Z , 1dZ 、 2dZ 、 3dZ 、 4dZ are the vertical displacement of the dynamic vibration absorber corresponding to the corresponding wheel is represented.        = r FF C q K q , (2)   0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 r r r r r C C C C C                                               0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 0 r r r r r K K K K K                                             , (3) Dynamic vibration absorber
  • 3. Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber www.ijres.org 14 | Page III. MODEL SOLVING The Fourier transform (1) is performed in the frequency domain:            12 H M j C K F          , (4) Since the excitation of each wheel has a certain delay, the input of the three wheel is considered as the input of the first wheel. Wheels by incentive matrix:    1 2 3 4 1( ) ( ) ( ) ( ) ( ) T q q q q Q q     , (5) In the formula: 1 ( )q  、 2 ( )q  、 3 ( )q  、 4 ( )q  respectively, the excitation of the four wheels in the frequency domain. Including:   32 4 = 1 Tj Tj T j T Q e e e      , (6) In the formula 2 2 tT l u , 3 2 cT l u ,  4 2 t cT l l u  . It can be obtained that the frequency response matrix of each part of the vehicle is not smooth, and each element of the matrix is the frequency response function of the displacement of the vehicle.          1 14= T h H Q h h              , (7) According to the frequency response function of the displacement, the acceleration response function can be obtained.        1 2 2 1 i i iZ q Z h h q           , (8)      1 1 2 1i i Z q Z q G h q      , (9) In the formula:   1iZ q h   is the acceleration frequency response function of the corresponding component relative to the irregularity excitation is expressed,   1iZ q G   is the acceleration power spectral density of the corresponding components for the irregularity excitation is indicated. Although the acceleration power spectral density can be very convenient to analyze the frequency characteristics of vertical vibration of vehicle system, the acceleration of vertical vibration of the vehicle in the frequency range of 1 to n frequency range is required:    1 1 2n ii zG G d          , (10) IV. SIMULATION RESULTS 4.1 MODEL PARAMETERS Based on one type of vehicle as an example, According to the dynamic vibration absorber principle can determine the dynamic vibration absorber absorbing quality and stiffness, the parameters are shown in Table 1, With American class six track irregularity spectrum as incentive of the vehicle vertical vibration model. Table1 A certain type of vehicle parameters and track parameters Meaning Parameter symbol Value Mass of vehicle Mb/kg 4.18×104 Car body pitch inertia Jb/(kg·m2) 1.686×106 Mass of bogie Mt/kg 2.8×103 Bogie pitch inertia Jt/( kg·m2) 1.93×103 Secondary spring stiffness per bigie Ks2/( kN·m-1) 6×105 Secondary damping per bogie Cs2/( kN·s·m-1) 1.1×104 Primary spring stiffness per axle Ks1/( kN·m-1) 1.11×106 Primary spring damping per axle Cs1/( kN·s·m-1) 2.4×104 Half of bogie centers lb/m 9 Half of bogie wheel base lw/m 1.25 Mass of Dynamic vibration absorber Md/kg 140 Dynamic vibration absorber stiffness Kd/( kN·m-1) 4×105 Dynamic vibration absorber damping Cd/( kN·s·m-1) 50
  • 4. Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber www.ijres.org 15 | Page 4.2 PERFORMANCE ANALYSIS OF DYNAMIC VIBRATION ABSORBER To simulate the model and obtain the components of the vehicle vertical vibration acceleration power spectral density. Fig.3 Effect of dynamic vibration absorber on the vibration of wheel set The wheel vertical acceleration power spectral density curves of vibration is as shown in Fig. 3, It can be seen from Fig. 3 that the wheel's vertical vibration at 40Hz with excitation frequency resonance and reached peak. Therefore, the wheel vibration is most intense, resulting in damage to the wheel strength, seriously affecting the safe operation of the vehicle. After installing the dynamic vibration absorber, vertical vibration of the wheel has been significantly reduced in the resonance frequency. Wheel vertical vibration is passed primary suspension up to the bogie, The wheel vibration directly affects the vibration situation of the bogie, the Front and rear bogie vertical acceleration power spectral density curves of vibration is as shown in Figure 4, It can be seen from Fig. 4 thatdue to the wheels produce resonance in 40Hz, leading to the bogie at 40Hz also produces vibration peak, dynamic vibration absorber reduce the vertical vibration of wheel at the resonant frequency, Vertical vibration transmitted to the bogie has been weakened, Therefore, the axle dynamic vibration absorber can not only reduce the wheel vertical vibration can also weaken the vertical vibration of the bogie. (a) Front bogie PSDofFrontbogie/m2s-3 f /Hz f /Hz PSDofWheelset/m2s-3 No DVA With DVA
  • 5. Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber www.ijres.org 16 | Page (a) Rear bogie Fig.4 The influence of dynamic vibration absorber on the vibration of bogie The car body vertical acceleration power spectral density curves of vibration is as shown in Fig. 5, It can be seen from Fig.5 that due to bogie vertical vibration in the vicinity of 40Hz is weakened, so the vertical vibration of the vehicle body vibration at this frequency is also weakened. However, the body's natural frequency of about 1.5Hz, body vertical vibration of the energy is concentrated at low frequencies near the natural frequency. The vibration energy is smaller in the near of 40Hz frequency. Therefore, although the dynamic vibration absorber can reduce vibration here, the effect of reduce the vehicle's vertical vibration is limited Fig.5 Effect of dynamic vibration absorber on the vibration of car body The wheel has a good vertical vibration damping effect on the wheel. In order to improve the vibration performance, the mass ratio of the dynamic vibration absorber is improved. Fig. 6 shows the influence of the mass ratio of the dynamic vibration absorber on the vibration absorption performance of the dynamic absorber. The mass ratio of the dynamic vibration absorber can obviously improve the vibration reduction performance. Moreover, the vibration frequency band of the dynamic vibration absorber is gradually widened. PSDofCarbody/m2s-3 f /Hz PSDofRearbogie/m2s-3 f /Hz
  • 6. Study on Vibration Reduction Effect of the Rail Vehicle with Axle Dynamic Vibration Absorber www.ijres.org 17 | Page Fig.6 Influence of mass ratio on the vibration reduction effect of dynamic vibration absorber V. CONCLUSIONS Axle vibration absorber for vertical vibration of the wheel not only has a good inhibition, but also on the bogie and the body has a important damping effect. For the vertical vibration of the vehicle body is mainly concentrated in the low frequencies, therefore, the axle dynamic vibration damping effect on the body is limited. The vibration reduction effect can be improved by increasing the mass ratio of the axle dynamic vibration absorber. The vibration of the wheel is radiated from the outside; therefore, the vibration of the axle can be controlled by reducing the vertical vibration of the wheel. VI. ACKNOWLEDGEMENTS The authors would like to acknowledge the support of National Natural Science Foundation of China (Grant No. 11472176), Natural Science Foundation of Shanghai (Grant No. 15ZR1419200) and Discipline Construction Project for Transportation Engineering (Grant No. 13SC002). REFERENCES [1] XU Zhisheng ZHAI Wanming Prediction and Control of Wheel/Rail Noise for Rail Transit [J].China Railway Science, 2006,27(1):138-139. [2] ZHAO Hong-lun YU Cheng-liang WANG Wen-bin. Study on Optimization Design of Carbody Structure of High-speed Maglev Train [J]. Journal of the China Railway Society, 2007,04:43-47. [3] FOO E,GOODALL R M.Active Suspension Control of Flexible-Bodied Railway Vehicle Using Electro-Hydraulic and Electromagnetic Actuators[J].Control Engineering Practice,2000,8:507-518. [4] ZENG Jing;WU Ping-bo;HAO Jian-hua.Analysis of Vertical Vibration Reduction for Railway Vehicle Systems [J]. China Railway Science, 2006,27(3):62-67. [5] ZHOU Jinsong ZHANG Wei SUN Wenjing .Vibration Reduction Analysis of the Dynamic Vibration Absorber on the Flexible Carbody of Railway Vehicles[J]. China Railway Science,2009,30(3):86-90. [6] ZHOU Jinsong GONG Dao REN Lihui.Simulation on Passive Vibration Control of Flexible Carbody of Railway Passenger Vehicles[J]. Journal of TongJi University (Natural Science),2009,37(8):1085-1089. [7] Takahiro Tomioka, Tadao Takigami. Reduction of bending vibration in railway vehicle carbodies using carbody–bogie dynamic interaction[J]. Vehicle System Dynamics.2010.4.467-486. No DVA μ=0.003 μ=0.015 f /Hz PSDofWheelset/m2s-3