1. 中国航发北京航空材料研究院钛合金研究所,北京,100095
2. 中国航发先进钛合金重点实验室,北京,100095
3. 清华大学新材料国际研发中心,北京,100084
纸质出版:2020
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弭光宝,梁贤烨,李培杰,曹京霞,黄旭 . 航空发动机钛合金在微尺度下摩擦着火特性数值计算分析[J]. 航空制造技术, 2020, 63(16): 68-74/85.
MI Guangbao, LIANG Xianye, LI Peijie,CAO Jingxia, HUANG Xu. Numerical Calculation and Analysis of Friction Ignition Characteristics of Aero-Engine Titanium Alloy at Micro-Scale. Aeronautical Manufacturing Technology, 2020, 63(16): 68-74/85.
弭光宝,梁贤烨,李培杰,曹京霞,黄旭 . 航空发动机钛合金在微尺度下摩擦着火特性数值计算分析[J]. 航空制造技术, 2020, 63(16): 68-74/85. DOI: 10.16080/j.issn1671-833x.2020.16.068.
MI Guangbao, LIANG Xianye, LI Peijie,CAO Jingxia, HUANG Xu. Numerical Calculation and Analysis of Friction Ignition Characteristics of Aero-Engine Titanium Alloy at Micro-Scale. Aeronautical Manufacturing Technology, 2020, 63(16): 68-74/85. DOI: 10.16080/j.issn1671-833x.2020.16.068.
叶片与机匣的异常摩擦是航空发动机钛火发生的主要热源。将航空发动机钛合金摩擦着火过程的微凸起 / 微碎片作为研究对象,建立考虑摩擦热源的微尺度着火模型,计算分析了粒径、摩擦系数、氧浓度和流速等因素的影响规律,并与经典模型进行比较。结果表明:临界着火温度及延迟时间随着粒径的减小不断降低,随着摩擦系数下降不断增大,随着氧浓度增加不断降低,随着流速的提高而呈上升趋势;当粒径为 82.5μm 时,经典模型与摩擦模型的临界着火温度分别为 825K 和 677K,着火延迟时间分别为 0.035s 和 0.032s ;当摩擦系数减小 0.2 时,其临界着火温度提高约 20K,而着火延迟时间提高约 10s ;当氧浓度为 50% 时,经典模型与摩擦模型的着火温度分别为 826K 和 782K ;当流速为 310m/s 时,经典模型与摩擦模型的着火温度分别为 966K 和 964K,着火延迟时间分别为 0.54s 和 0.43s。
The abnormal friction between the vane and the casing is the main heat source of titanium fire in the aero-engine. In this paper
micro-protrusion / micro-debris of aero-engine titanium alloy friction ignition process is taken as the research object
a micro-scale ignition model considering friction heat source is established
and the influence rules of particle size
friction coefficient
oxygen concentration and flow velocity are calculated and analyzed
and compared with the classic model. The results show that the critical ignition temperature and delay time continue to decrease with decreasing particle size
increase with decreasing friction coefficient
decrease with increasing oxygen concentration
and increase with increasing flow velocity; When the particle size is 82.5μm
the critical ignition temperature of the classic model and friction model are 825K and 677K
respectively
and the ignition delay time is 0.035s and 0.032s respectively; when the friction coefficient decreases by 0.2
the critical ignition temperature increases by about 20K
the ignition delay time increase by about 10s; when the oxygen concentration reached 50%
the ignition temperatures of the classic model and friction model are 826K and 782K
respectively; when the flow velocity is 310m/s
the critical temperatures of the classic model and friction model are 966K and 964K
respectively
the ignition delay time is 0.54s and 0.43s respectively.
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