TC4钉体内螺纹深孔攻丝仿真研究

Simulation study of deep hole tapping in TC4 rivet body threads

  • 摘要: 钉体作为航空用钛合金平断面大底脚螺纹抽钉的主要承力部件,其研制过程中的内螺纹成形工艺控制是重难点。针对TC4钉体内螺纹深孔攻丝成形工艺,通过有限元仿真分别研究钉体和丝锥在攻丝过程中的受力特点,建立丝锥所受扭矩与行程的关系模型,并结合参数仿真研究关键工艺参数对丝锥受力的影响规律。结果表明,丝锥切削刃旋出后,钉体内最大等效应力约为切削阶段的10.12%;等效应变分布区域随着攻丝过程的进行逐渐增大,已成形螺纹段所受平均等效应变大于正在成形螺纹段;丝锥在切削阶段的扭矩模型预测值与各仿真试验组的计算值误差均在10%以内;随着底孔直径从2.78增大至2.90 mm,攻丝过程平均扭矩从372.762 8减小至292.224 2 N∙mm;随着剪切摩擦因数从0.2增大至1.0,攻丝过程平均扭矩从313.099 3增大至427.203 9 N∙mm;随着旋进速度从1.75减小至1.05 mm/s,攻丝过程平均扭矩从373.072 2减小至334.333 7 N∙mm。

     

    Abstract: The rivet body is the main load-bearing part of the aerospace titanium alloy flat-section large base foot threaded blind rivets. Controlling the internal thread forming process during development is a critical challenge. For the deep hole tapping and forming process of TC4 rivet body, the force characteristics of the rivet body and tap in the tapping process are studied by finite element simulation, the relationship model between the torque and stroke of the tap is established, and the influence of key process parameters on the tapping force is studied by combining with parametric simulation. The results show that after the tap cutting edge is rotated out, the maximum effective stress in the rivet body is about 10.12% of the cutting stage. The distribution area of the effective strain field gradually increases with the tapping process, and the average effective strain of the formed thread section is greater than that of the thread section being formed. The torque prediction of the tap in the cutting stage and the calculated value of each simulation test group have an error of less than 10%. As the base hole diameter increased from 2.78 to 2.90 mm, the average torque of the tapping process decreased from 372.762 8 to 292.224 2 N∙mm. As the shear friction coefficient increased from 0.2 to 1.0, the average torque of the tapping process increased from 313.099 3 to 427.203 9 N∙mm. As the work-in speed decreased from 1.75 to 1.05 mm/s, the average tapping torque decreased from 373.072 2 to 334.333 7 N∙mm.

     

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