• Title/Summary/Keyword: Low Frequency Brake Squeal Noise

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A Study on the Squeal Noise Instability Analysis on Caliper Brake (캘리퍼 브레이크 스퀼 소음의 불안정성 해석에 관한 연구)

  • Lee, Junghwan;Kim, Seonghwan
    • Transactions of the Korean Society for Noise and Vibration Engineering
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    • v.23 no.11
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    • pp.957-965
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    • 2013
  • This paper deals with analytical methods for low frequency and high frequency brake squeal noise on brake-rear caliper. In order to improve low frequency and high frequency squeal noise, we take survey caliper bracket shape parameters and housing shape parameters. Besides, using the combination of bracket and housing parameter were surveyed. Thus, using the combination of bracket Alt_05 and housing Alt_45 specifications, instability analysis and brake dynamo test were carried out. Based upon the two models, low and high frequency squeal noise of base model were improved. But, for 6.0 kHz frequency noise, which is not improved, it needs to additionally study on instability analysis and combination of the other brake components.

Analysis and Evaluation of the Brake NVH Characteristics for the Fusion-type Friction Material (퓨전형 마찰재의 브레이크 NVH 특성 해석 및 평가)

  • Kwon, Seong-Jin;Bae, Chul-Yong;Kim, Chan-Jung;Kim, Wan-Soo;Lee, Dong-Won;Lee, Bong-Hyun;Seo, Byoung-Youn;Jung, Kwang-Ki
    • Proceedings of the Korean Society for Noise and Vibration Engineering Conference
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    • 2008.11a
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    • pp.606-607
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    • 2008
  • Nowadays, noise and vibration phenomena of a disc brake system have been given various names that provide some definitions of sound and vibration emitted such as grind, grunt, moan, squeak, squeal, judder and wire brush. The most common and annoying noise of a disc brake system is squeal noise. It is defined as noise whose frequency content is 1 kHz and higher with excessively high and irrigating sound pressure levels. In this paper, the noise and vibration characteristics of a disc brake system have been investigated to develop the fusion-type friction material, which overcomes the low steel and non-asbestos organic friction materials. For the purpose, both experimental evaluation and complex eigenvalue analysis have been carried out.

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Factor Effects of Low-Frequency Instability of Brake System Using Complex Eigenvalue Analysis (복소 고유치 해석을 통한 브레이크 시스템의 저주파 불안정성 영향인자 분석)

  • Lee, Ik Hwan;Jeong, Wontae;Park, Kyung Hwan;Lee, Jongsoo
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.38 no.6
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    • pp.683-689
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    • 2014
  • The present study conducted a parameter effect analysis of low-frequency squeal noise using a numerical simulation. The finite element program ABAQUS was used to calculate the dynamic instability based on a complex eigenvalue analysis. A total of five parameters, including the chassis, wear, piston, material property, and contact condition, were selected to identify the factor effects on a low-frequency squeal noise between 2.5 and 3.1 kHz. The present study found the dominant level of each factor through an analysis of the means in the context of the experiment design.

Low Frequency Squeal Noise Reduction using Mode Participation Factor in Complex Eigenvalue Analysis (복소고유치해석에서 모드기여도 인자를 이용한 저주파 스퀼소음 저감)

  • Park, Jeong Min;Kim, Hyun Soo;Yoon, Moon Young;Boo, Kwang Seok;Kim, Heung Seob
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.37 no.3
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    • pp.325-331
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    • 2013
  • In this study, a complex eigenvalue analysis is implemented to verify the unstable mode of a brake system using ABAQUS software. The component participation factors and component modal participation factors are used to analyze the total contributions from each component and each component mode to a particular unstable system mode. This study shows that the 1.4-kHz unstable system mode comes from mode coupling between the 2nd nodal diametric mode and 3rd lateral axial mode (LAM) in the baseline model. A sensitivity analysis with a linking index is performed to prevent the mode coupling of the component modes. This linking index analysis shows the optimum mass loading position to move away the natural frequency of the 3rd LAM, which contributes to the unstable mode. Finally, a complex eigenvalue analysis is implemented with mass loading in the tie bar position, and no unstable system mode is generated in the low-frequency range (below 2 kHz).