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    贾剑平, 骆敏, 李虹钢. 冷金属过渡电弧增材制造高强钢过程中温度场的数值模拟[J]. 机械工程材料, 2024, 48(7): 100-107. DOI: 10.11973/jxgccl230245
    引用本文: 贾剑平, 骆敏, 李虹钢. 冷金属过渡电弧增材制造高强钢过程中温度场的数值模拟[J]. 机械工程材料, 2024, 48(7): 100-107. DOI: 10.11973/jxgccl230245
    JIA Jianping, LUO Min, LI Honggang. Numerical Simulation of Temperature Field in Cold Metal Transfer Arc Additive Manufacturing High-Strength Steel[J]. Materials and Mechanical Engineering, 2024, 48(7): 100-107. DOI: 10.11973/jxgccl230245
    Citation: JIA Jianping, LUO Min, LI Honggang. Numerical Simulation of Temperature Field in Cold Metal Transfer Arc Additive Manufacturing High-Strength Steel[J]. Materials and Mechanical Engineering, 2024, 48(7): 100-107. DOI: 10.11973/jxgccl230245

    冷金属过渡电弧增材制造高强钢过程中温度场的数值模拟

    Numerical Simulation of Temperature Field in Cold Metal Transfer Arc Additive Manufacturing High-Strength Steel

    • 摘要: 基于冷金属过渡(CMT)高频熄弧的特性,在双椭球热源模型的基础上建立了动态热源模型,采用ABAQUS软件建立了高强钢CMT电弧增材制造单道十层成形件的有限元模型,对成形过程中的温度场进行模拟,并与试验结果进行对比;采用模拟方法研究了层间冷却时间(30,60,90 s)和基板预热温度(20,200,300 ℃)对温度场的影响规律。结果表明:模拟得到基板表面距焊道中心20.5 mm处的热循环曲线的变化趋势与试验结果基本一致,波峰和波谷温度的相对误差均在10%以内,证明了模型的准确性。沉积下一层时仅对前一层起到重熔作用;在沉积过程中,熄弧端的峰值温度高于起弧端,而在冷却过程中,两端温度差逐渐降低。随着层间冷却时间的延长,熔池最高温度降低且熔池存在的时间变短,在冷却阶段的冷却速率增大但其增大的程度降低,成形件两端温度差降低,最佳层间冷却时间为90 s;随着基板预热温度的升高,熔池的最高温度和熔池尺寸均增加,最大波谷温度差先减小后增大,在基板预热200 ℃条件下,成形件的最大波谷温度差最小,温度分布更加均匀。

       

      Abstract: Based on the high-frequency extinguishing characteristics of cold metal transfer (CMT), a dynamic heat source model was established on the basis of the double ellipsoid heat source model. The finite element model of high-strength steel CMT arc additive manufacturing single-pass ten-layer formed part was established by ABAQUS software. The temperature field during the forming was simulated and compared with test results. The influence of interlayer cooling time (30, 60, 90 s) and substrate preheating temperature (20, 200, 300 ℃) on the temperature field was studied by the simulation method. The results show that the trend of the thermal cycle curve at the position 20.5 mm from the center of weld bean on surface of the substrate was basically consistent with the test results, and the relative errors of peak and valley temperatures were both less than 10%, which proved the accuracy of the model. Only the previous layer remelted when the next layer was deposited. During the deposition, the peak temperature of the arc extinguishing end was higher than that of the arc starting end, but the temperature difference between the two ends decreased during cooling. With the extension of interlayer cooling time, the maximum temperature of the molten pool decreased and the existing time of the molten pool became shorter; the cooling rate increased in the cooling stage, but the increase degree decreased the temperature difference between the two ends of the formed part was reduced. The optimum interlayer cooling time was 90 s. With the increase of substrate preheating temperature, the maximum temperature and the size of the molten pool increased, and the maximum valley temperature difference decreased first and then increased. Under the condition of preheating 200 ℃ of the substrate, the maximum valley temperature difference of the formed parts was the smallest, and the temperature distribution was more uniform.

       

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