• Title/Summary/Keyword: Transient Chip Formation

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Transient Chip Formation in Cutting with a Self-propelled Rotary Tool (자기추진 로타리 공구를 사용한 절삭에서 천이 칩의 형성)

  • 최기흥;최기상
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.17 no.5
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    • pp.1041-1053
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    • 1993
  • A theoretical model to predict the triangular chip formation in cutting with a self-propelled rotary tool is developed. The model is based on the model of transient chip formation in two dimensional orthogonal cutting. The predicted results are found to be in good agreement with the experimental observations and suggest that transient charcteristics of work material, which depend on both cutting conditions and material properties, have the significant influence on triangulation.

A Study on Transient Chip Formation in Cutting with Self-Propelled Rotary Tools-Experimental Verification (자기추진 로타리 공구를 사용한 절삭에서 천이칩 형성에 관한 연구 - 실험에 의한 증명)

  • 최기흥;최기상;김정수
    • Transactions of the Korean Society of Mechanical Engineers
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    • v.17 no.8
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    • pp.1910-1920
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    • 1993
  • An experimental study to investigate the unconventional chip formation called triangulation of chip in cutting with a SPRT (self-propelled rotary tool) is performed using acoustic emission (AE) signal analysis. In doing that, a quantitative model of the AE RMS signal in triangulation with a SPRT is first developed. The predicted results from this model show good correlation between the AE RMS signal and the general characteristics of triangular chip formation. Then, effects of various process parameters such as cutting conditions (cutting speed, depth of cut, oblique angle and normal rake angle) and the work material properties on the chip formation in cutting with a SPRT are explored. Special attention is paid to the work material properties which are found to have significant effects on triangulation.

Round Jet Impingement Heat Transfer on a Pedestal Encountered in Chip Cooling (원형 충돌제트를 이용한 Pedestal 형상의 핀이 부착된 Chip 냉각)

  • Chung, Young-Suk;Chung, Seung-Hoon;Lee, Dae-Hee;Lee, Joon-Sik
    • Proceedings of the KSME Conference
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    • 2001.06d
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    • pp.546-552
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    • 2001
  • The heat transfer and flow measurements on a pedestal encountered in chip cooling. A uniform wall temperature boundary condition at the plate surface and on a pedestal was created using shroud method. Liquid crystal was used to measure the plate surface temperature. The jet Reynolds number (Re) ranges from 11,000 to 50,000, the dimensionless nozzle-to-surface distance (L/d) from 2 to 10, and the dimensionless pedestal diameter-to-height (H/D) from 0 to 1.0. The results show that the Nusselt number distributions at the near the pedestal exhibit secondary maxima at $r/d{\cong}1.0\;and\;1.5$. The formation of the secondary maxima is attributed to an create in the vortex by the pedestal.

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Jet Impingement Heat Transfer on a Cylindrical Pedestal Encountered in Chip Cooling (충돌제트를 이용한 Pedestal 형상의 칩 냉각연구)

  • Lee, Dae-Hee;Lee, Joon-Sik;Chung, Young-Suk;Chung, Seung-Hoon
    • Transactions of the Korean Society of Mechanical Engineers B
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    • v.27 no.1
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    • pp.1-8
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    • 2003
  • The heat transfer and flow measurements on a cylindrical pedestal mounted on a flat surface with a turbulent impinging jet were made. The experiments were made for the jet Reynolds number of Re = 23,000, the dimensionless nozzle-to-surface distance of L/d = 2~10, the dimensionless pedestal height of H/D = 0~1.5. Measurements of the surface temperature and the Nusselt number distributions on the plate surface were made using liquid crystal and shroud-transient technique. Flow measurements involve smoke flow visualization and the wall pressure coefficient. The results show that the wall pressure coefficient sharply decreases along the upper surface of the pedestal. However, the pressure increases when the fluid escapes from the pedestal and then collides on the plate surface. The secondary maxima in the Nusselt numbers occur in the region of 1.0 $\leq$ r/d $\leq$ 1.9. Their values for the case of H/D = 0.5 are maximum 80% higher than those for other cases. The formation of the secondary maxima may be attributed to the reattachment of flow on the plate surface which was separated at the edge of the pedestal.