供油孔流量数值模拟及其飞秒激光加工工艺优化

Numerical simulation of oil supply holes flow and optimization of its femtosecond laser processing technology

  • 摘要: 航天发动机供油装置的喷油流量均匀性是决定其性能质量的关键技术指标,其中供油孔的形状尺寸、内表面状态是喷油流量的重要影响因素。传统的供油孔加工方法以电火花加工为主,存在较厚的重铸层,且加工效率低。而激光制孔为典型的非接触式制孔方法,具有加工效率高、质量好,重铸层少的显著优势。为满足某型号航天发动机供油装置的高效高质量制造要求,采用脉宽为200 fs的超短脉冲飞秒激光螺旋制孔工艺,针对1.5 mm厚的GH3044镍基合金材料开展了以0.39 mm孔径为加工基准的流量数值模拟及工艺试验研究。首先通过数值模拟手段,研究了孔径、圆度、锥度以及内壁粗糙度对供油孔流量的影响规律和控制手段,之后根据模拟所获得的理论结果,通过飞秒激光制孔试验对制孔工艺进行了优化。研究发现,出入口孔径是决定流量大小最重要的因素,在单脉冲能量140 μJ,单层扫描时间1200 ms,单层进给量0.02 mm,重复频率100 kHz,旋转速度2400 r/min的工艺下,将孔径偏差控制在±5 μm以内,最终成功实现了供油孔流量偏差1.8%的制孔效果。

     

    Abstract:
      Objective   The uniformity of oil injection flow of the aerospace engine oil supply device is a key technical index to determine its performance quality, in which the shape and size of the injection hole and the state of the internal surface are important influencing factors of the oil injection flow. The traditional oil injection hole processing method is based on EDM, there is a thick recast layer, and the processing efficiency is low. The laser hole is made with a typical non-contact hole making method, which has significant advantages of high processing efficiency, good quality and less recast layer. In order to meet the high-efficiency and high-quality manufacturing requirements of a certain type of aerospace engine fuel supply device, the ultra-short pulse femtosecond laser screw hole making process with a pulse width of 200 fs was adopted, and the flow numerical simulation and process test study with 0.39 mm hole diameter as the processing benchmark were carried out for the 1.5 mm thick GH3044 nickel-based alloy material.
      Methods  By means of numerical simulation, the effect of hole diameter (Fig.6), taper (Fig.8), roundness (Fig.9), internal wall roughness (Tab.2) and hole depth (Fig.10) on the flow rate of oil supply hole is studied. The effect of single pulse energy (Fig.13), single layer scan time (Fig.14) and single layer feed (Fig.15) on the hole diameter is analyzed, and the hole diameter deviation is controlled by process optimization to ensure the flow stability.
      Results and Discussions  Numerical simulations were used to investigate the factors influencing the hole flow rate. The results show that the hole diameter is the main factor affecting the hole flow rate, and the flow rate is linearly related to the square of the hole diameter (Fig.6). The internal wall roughness has an inhibitory effect on the flow rate of holes. For a 0.39 mm diameter micro-hole, the flow rate is reduced by 3.3% when the roughness is 0.01 mm and by 5.96% when the roughness is 0.05 mm (Tab.2). The roundness (Fig.9) and height (Fig.10) of the micro-hole had no significant effect on the flow rate. Since the hole internal wall roughness of the femtosecond laser hole making was low and did not change significantly for different process parameters, only the effects of single pulse energy, single layer scan time and single layer feed on the micro-hole diameter were investigated. The process optimization was carried out according to the effect law of different process parameters on the micro-hole diameter. Using the optimized process for drilling, the maximum deviation of micro-hole water flow rate is finally less than 1.8% to meet the usage requirements.
      Conclusions   In this paper, the influence law of micro-hole quality on water flow is studied by numerical simulation. The micro-hole flow rate is mainly determined by the diameter of the hole entrance and exit. Under the premise of the same entrance and exit hole diameter, the depth and roundness of the hole have basically no effect on the hole flow rate. The larger the roughness of the internal wall of the micro-hole is, the smaller the flow rate is. The smaller the hole diameter is, the more significant the effect of roughness is. When the roughness height is 0.01 mm, the flow rate of 1 mm diameter is reduced by 0.32%, and the flow rate of 0.39 mm diameter is reduced by 3.30%. The effect of process parameters on the micro-hole diameter was analyzed. With the increase of single pulse energy, the entrance and exit hole diameter increased simultaneously and the taper decreased. The effects of single layer scan time and single layer feed on hole diameter were not significant. Finally, the deviation of the hole diameter was controlled within ±5 μm and the taper was 0.01° by process optimization. The water flow rate test was conducted, and the maximum flow rate was 3.28 g/s, the minimum flow rate was 3.17 g/s, and the average flow rate was 3.23 g/s with a maximum deviation of 1.8%, which satisfied the usage requirements.

     

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