Journal of Jilin University(Engineering and Technology Edition) ›› 2023, Vol. 53 ›› Issue (10): 2741-2751.doi: 10.13229/j.cnki.jdxbgxb.20211344

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Effects of porous sound absorbing materials on tire cavity noise

Jian YANG1(),Hui-yun LI1,Hai-chao ZHOU1(),Guo-lin WANG1,Ling-xin ZHANG2   

  1. 1.School of Automotive and Traffic Engineering，Jiangsu University，Zhenjiang 212013，China
    2.AEOLUS Tyre Co. ，Ltd. ，Jiaozuo 454003，China
  • Received:2021-12-07 Online:2023-10-01 Published:2023-12-13
  • Contact: Hai-chao ZHOU E-mail:yangjian@ujs.edu.cn;hczhou@ujs.edu.cn

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Abstract:

A passenger car tire 205/55R16 is taken as the research object， and the relationship between tire force transmissibility and tire cavity resonance noise is studied through experiments. It is proposed that the amplitude of tire force transmissibility has the ability of representing the level of tire resonance cavity noise. A tire force transmissibility simulation model with sound-absorbing material is established using finite element method， and it is found that the mechanical parameters of porous sound-absorbing material have more significant influence on the noise reduction effect than the sound absorption coefficient. The optimal Latin hypercube test method and the Kriging approximate model are selected to explore the influences of the density， elastic modulus， width and thickness of the porous material's on the amplitude of the tire force transmissibility， and the multi-island genetic optimization algorithm is chosen to optimize the above four parameters of the porous material. By changing the single width parameter of the porous material， the accuracy of the simulation results is verified through the tire force transmission test and the falling noise test. The results show that compared with the original tire， the amplitude of tire force transmissibility of the optimized tire is significantly reduced， and the cavity resonance noise of the tire is also effectively improved.

Key words: vehicle engineering, porous sound absorbing materials, tire force transmissibility, cavity resonance noise, simulation model

CLC Number: 

  • U463

Fig.1

Porous sound absorbing materials stickedon inner"

Table 1

Test instruments and functions"

仪器型号与名称用途
Endevco7703A?50型加速度传感器采集加速度信号
QT1125 4 LMS数据多通道采集仪采集激励信号
LMS Test. Lab 11B采集系统信号采集和处理
PCB086C04力锤施加冲击激励
直径1 cm的橡皮绳悬挂轮胎

Fig.2

Diagram of tire force transmissibility test"

Fig.3

Different tire force transmissibility test results"

Fig.4

Drum test for tire noise"

Fig.5

Results of tire noise test"

Table 2

Force transmissibility amplitudes and noise values"

材料2号传声器/dB轮胎力传递率幅值/dB
未添加70.319.5
聚酯66.7-1.28
橡塑69.14.82
三聚氰胺63.3-2.94

Fig.6

Model of rim"

Fig.7

Tire model with porous sound absorbing materials"

Fig.8

Position of tire excitation force"

Table 3

Modal frequencies of different models"

内腔状空气模型无空气的轮胎模型耦合空气的轮胎模型
模态频率/Hz-207.9207.8
-209.2209.1
-224.6224.4
225.4-225.5
232.0-231.0
-238.7238.6
-251.3251.1
-252.4252.2

Fig.9

Frequency of air cavity"

Fig.10

Comparisons of rim accelerations using different models"

Fig.11

Comparisons of force transmissibility usingdifferent absorbing materials"

Table 4

Results comparisons between test and simulation"

材料力传递率试验/dB力传递率仿真/dB
未添加19.5-17.5671
橡塑4.82-17.6981
聚酯-1.28-17.8775
三聚氰胺-2.94-18.4741

Fig.12

Sound absorption coefficients of the twoPolyurethane materials"

Fig.13

Compress tests of two polyurethane materials"

Fig.14

Two different sound absorption materials"

Fig.15

Comparisons of sound absorption coefficients"

Fig.16

Parameters of sound absorption materials"

Table 5

Test schemes and simulation results"

试验方案ρ/（kg·m-3）C10b/cmh/cm力传递率峰值/（m·s-2）
113.00550.1589.111.2630.018 568 3
214.47562.00010.211.9470.016 754 0
315.95443.57910.581.2110.016 313 3
417.42408.05311.681.8420.011 619 1
518.89348.84212.051.0530.012 504 9
620.37490.9478.001.5790.016 352 7
721.84538.31613.891.8950.015 151 6
823.32337.00012.791.1580.014 457 1
924.79372.52612.421.3680.008 619 9
1026.26455.42114.261.3160.011 703 2
1127.74479.10513.531.0000.011 304 3
1229.21514.6328.371.6320.015 865 2
1330.68502.78914.631.6840.009 895 7
1432.16431.73715.001.4210.012 647 5
1533.63384.36811.321.7890.014 111 0
1635.11419.8959.471.5260.013 713 6
1736.58467.2638.741.1050.008 592 1
1838.05526.47413.162.0000.015 911 4
1939.53396.2119.841.4740.015 737 3
2041.00360.68410.951.7370.011 008 9

Fig.17

Precision prediction for Kriging model"

Table 6

Verification of the Kriging model"

A/（kg·m-3）BC/cmD/cm预测值/（m·s-2）仿真值/（m·s-2）误差
274501520.012 520.011 349.4%
32.552012.41.240.013 470.012 785.1%

Table 7

Parameters values before and after the optimized"

项目因子
A/（kg·m-3）BC/cmD/cm
优化前27445121.5
优化后27.452370.8612.5761.3843

Fig.18

Contribution analysis of each parameter"

Fig.19

Contribution analysis of composite parameters"

Fig.20

Effects of different widths on force transmissibility"

Fig.21

Effects of different widths on tire drop noise"

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