• Title/Summary/Keyword: 테이퍼 롤러 베어링 케이지

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Analysis of Dynamic Characteristics for a Tapered Roller Bearing Cage (테이퍼 롤러 베어링 케이지의 동특성 해석)

  • Park, Jang-Woo;Heo, Jun-Young
    • Journal of the Korea Convergence Society
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    • v.8 no.5
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    • pp.179-184
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    • 2017
  • The cage of a tapered roller bearing keeps the gap between the rollers, which prevents friction, wear and suppresses heating. The material of the cage is changing from metal to plastic for lightening the weight. If the cage is severely deformed due to resonance, the roller may not be able to roll and even get off the cage. In this paper, the dynamic characteristics of the cage is analyzed according to the cage material. Under the assumption that a train runs at the highest speed, frequency harmonics of that speed is calculated, and the comparative analysis is carried out in order to select the optimum thickness of the cage, which is easy to change among the cage design variables for avoiding the resonance.

The Effects of Geometrical Imperfections on the Dynamic Characteristics of a Tapered Roller Bearing Cage (테이퍼 롤러 베어링 케이지의 불완전성이 통특성에 미치는 영향)

  • Ahn, Tae-Kil;Park, Jang-Woo
    • Journal of the Korea Academia-Industrial cooperation Society
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    • v.20 no.4
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    • pp.464-469
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    • 2019
  • Tapered roller bearings are used widely in vans, trucks, and trains because they can support the vehicle in a stable manner even under a heavy load. The cage of a tapered roller bearing maintains the gap between the rollers, which prevents friction wear and suppresses heating. If the cage is severely deformed due to resonance, the roller may not be able to roll smoothly and even leave the cage. Consequently, it is very important to analyze the dynamic characteristics of the cage for reliable performance of a bearing. The cage essentially has geometrical tolerance in the manufacturing process. In this paper, the effects of those geometrical imperfections on the dynamic characteristics of the cage were investigated. As a result, natural frequency separation occurred near the natural frequency of the ideal cage due to geometrical imperfections. In addition, the interval was proportional to the magnitude of the geometric error, and the interval increased with increasing mode number.