中国物理B ›› 2016, Vol. 25 ›› Issue (12): 124601-124601.doi: 10.1088/1674-1056/25/12/124601

• ELECTROMAGNETISM, OPTICS, ACOUSTICS, HEAT TRANSFER, CLASSICAL MECHANICS, AND FLUID DYNAMICS • 上一篇    下一篇

Lubricant film flow and depletion characteristics at head/disk storage interface

Hong-Rui Ao(敖宏瑞), Zhi-Ying Han(韩志英), Kai Zhang(张凯), Hong-Yuan Jiang(姜洪源)   

  1. School of Mechatronics Engineering, Harbin Institute of Technology, Harbin 150001 China
  • 收稿日期:2016-05-05 修回日期:2016-08-04 出版日期:2016-12-05 发布日期:2016-12-05
  • 通讯作者: Hong-Rui Ao E-mail:hongrui_ao@hit.edu.cn
  • 基金资助:

    Project supported by the National Natural Science Foundation of China (Grant No. 51275124).

Lubricant film flow and depletion characteristics at head/disk storage interface

Hong-Rui Ao(敖宏瑞), Zhi-Ying Han(韩志英), Kai Zhang(张凯), Hong-Yuan Jiang(姜洪源)   

  1. School of Mechatronics Engineering, Harbin Institute of Technology, Harbin 150001 China
  • Received:2016-05-05 Revised:2016-08-04 Online:2016-12-05 Published:2016-12-05
  • Contact: Hong-Rui Ao E-mail:hongrui_ao@hit.edu.cn
  • Supported by:

    Project supported by the National Natural Science Foundation of China (Grant No. 51275124).

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摘要：

The characteristics of lubricant film at head/disk interface (HDI) are essential to the stability of hard disk drives. In this study, the theoretical models of the lubricant flow and depletion are deduced based on Navier-Stokes (NS) and continuity equations. The air bearing pressure on the surface of the lubrication film is solved by the modified Reynolds equation based on Fukui and Kaneko (FK) model. Then the lubricant film deformations for a plane slider and double-track slider are obtained. The equation of lubricant film thickness is deduced with the consideration of van der Waals force, the air bearing pressure, the surface tension, and the external stresses. The lubricant depletion under heat source is simulated and the effects of different working conditions including initial thickness, flying height and the speed of the disk on lubricant depletion are discussed. The main factors that cause the lubricant flow and depletion are analyzed and the ways to reduce the film thickness deformation are proposed. The simulation results indicate that the shearing stress is the most important factor that causes the thickness deformation and other terms listed in the equation have little influence. The thickness deformation is dependent on the working parameter, and the thermal condition evaporation is the most important factor.

关键词: lubricant film, depletion, deformation characteristics, head/disk interface

Abstract:

The characteristics of lubricant film at head/disk interface (HDI) are essential to the stability of hard disk drives. In this study, the theoretical models of the lubricant flow and depletion are deduced based on Navier-Stokes (NS) and continuity equations. The air bearing pressure on the surface of the lubrication film is solved by the modified Reynolds equation based on Fukui and Kaneko (FK) model. Then the lubricant film deformations for a plane slider and double-track slider are obtained. The equation of lubricant film thickness is deduced with the consideration of van der Waals force, the air bearing pressure, the surface tension, and the external stresses. The lubricant depletion under heat source is simulated and the effects of different working conditions including initial thickness, flying height and the speed of the disk on lubricant depletion are discussed. The main factors that cause the lubricant flow and depletion are analyzed and the ways to reduce the film thickness deformation are proposed. The simulation results indicate that the shearing stress is the most important factor that causes the thickness deformation and other terms listed in the equation have little influence. The thickness deformation is dependent on the working parameter, and the thermal condition evaporation is the most important factor.

Key words: lubricant film, depletion, deformation characteristics, head/disk interface

中图分类号:  (Tribology and mechanical contacts)

  • 46.55.+d
47.15.gm (Thin film flows) 68.03.-g (Gas-liquid and vacuum-liquid interfaces)