ISSN   1004-0595

CN  62-1224/O4

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3J1与G95Cr18配副在15#航空液压油润滑下的摩擦学行为

Tribological behavior of 3J1 paired G95Cr18 under 15# aviation hydraulic oil lubrication

  • 摘要: 随着航空工业液压件对更高转速、载荷及温度的需求,亟需开发出1种全新的摩擦磨损材料体系. 本文中通过选择Ni36CrTiAl (3J1)与G95Cr18配副,通过使用UMT5多功能摩擦磨损试验机,探究其在15#航空液压油中的摩擦学行为. 结果表明:随着速度的增加,该体系的摩擦系数呈现出先增加后减小再增加的趋势,磨斑直径呈现逐渐增加的趋势;该体系随着载荷的增加,也呈现出和速度增加时相同的趋势;最后探究了温度对该体系摩擦性能的影响,摩擦系数随着温度的增加呈现出先减小后增加再减小的趋势. 当速度为75 mm/s,载荷为5 N,温度为室温时,此时的摩擦性能最佳. 通过X射线光电子能谱(XPS)探究此时的摩擦机理,结果发现此时的摩擦区域形成一层反应氧化膜,此氧化膜是高性能摩擦磨损的关键. 该体系的研究从摩擦学方面为新一代航空领域材料的研究提供了理论指导.

     

    Abstract: The aviation industry is increasingly demanding higher speeds, loads, and temperatures, necessitating the urgent development of a new friction and wear system. This article examines the tribological behavior of Ni36CrTiAl (3J1) and G95Cr18 in 15# aviation hydraulic oil. We selected a pair and employed a UMT5 multifunctional friction and wear tester for the study. Our results indicated that as speed increased, the system’s friction coefficient initially rises, then falls, before rising again. Concurrently, the wear scar diameter steadily increased. As the speed increased, the friction coefficient of the system increased from 0.103 (10 mm/s) to 0.122 (30 mm/s), then decreased to 0.095 (75 mm/s), and finally increased to 0.101 (100 mm/s). When 3J1 and G95Cr18 were lubricated with 15# aviation hydraulic oil, the friction coefficient was at its minimum of only 0.095 when the rotational speed was at 75mm/s. This indicated that the lubrication conditions for this system were optimal under these circumstances. A long-wear experiment was conducted for 30 minutes under conditions of 5N, 75mm/s, and room temperature, followed by testing the friction coefficient of the system at different speeds. The results revealed that as the speed increases, the system enters a state of mixed lubrication. Observations from the microscope showed that as the speed increased, the carbon film gradually wears away and a new friction reaction film gradually forms at a rate faster than its consumption. Therefore, the friction coefficient was at its lowest at this point, but the wear scar enlarged. Calculations from 3D-light topography interferometer data showed that the wear rate was at its lowest at 75mm/s, being only 4.1×10-7 mm3/(N·m). As the speed changed, the primary wear mechanisms were abrasive wear and adhesive wear. The system exhibited the same trend with increased load as it does with increased speed. As the load increased, the friction coefficient of the system increased from 0.092 (1 N) to 0.133 (3 N), then decreased to 0.095 (5 N), and finally increased to 0.102 (10 N). Additionally, a long-wear experiment was conducted for 30 minutes under conditions of 5N, 75mm/s, and room temperature, followed by testing the friction coefficient of the system at different loads. The results showed that as the load increased, the system remained in a state of mixed lubrication. As the load increased, the wear rate gradually decreased. When the load is 10N, the wear rate was at its lowest, being only 9.8×10−8 mm3/(N·m). As the load changed, the primary wear mechanisms remained abrasive wear and adhesive wear. We also investigated the impact of temperature on the system’s friction performance. The friction coefficient showed a trend of first decreasing, then increasing, and then decreasing with the increase of temperature. As the temperature increased, the friction coefficient of the system increased from 0.095 (room temperature) to 0.131 (95 ℃) and finally decreased to 0.107 (155 ℃). This was due to the formation of carbides in the contact area, which significantly reduced the friction coefficient and fluctuates greatly. The friction coefficient showed a trend of first decreasing, then increasing and then decreasing again as the temperature increased. Notably, when the temperature rises to 155℃, 15# aviation hydraulic oil carbonized, and the generated carbon benefited friction wear. However, the consumption of carbon intensifies the friction in the wear area, therefore the friction coefficient began to rise again. When the temperature was at 75℃, the wear rate was at its lowest, being only 4.3×10−8 mm3/(N·m), which was 13.9% of the wear rate at 35℃. As the temperature changed, the primary wear mechanisms were abrasive wear and adhesive wear, and as the temperature rose, the characteristics of adhesive wear became more apparent. Optimal friction performance was achieved when the speed was 75 mm/s, the load was 5N, and the temperature was at room level. Further exploration of the friction mechanism via X-ray photoelectron spectroscopy (XPS) revealed the formation of a reactive oxide film in the friction area. This was key to achieving high-performance friction and wear. Our study provided theoretical guidance from a tribological perspective for material research in the next generation of aviation.

     

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