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感应钎焊细粒度金刚石粉末残余应力有限元分析

Finite element analysis of residual stress in fine-grained diamond powder during induction brazing

  • 摘要: 细粒度金刚石微粉因破损形状不规则,与钎料之间线膨胀系数差异较大,钎焊时在金刚石工具界面处极易产生残余应力,严重影响工具的加工使用性能.为了详细分析金刚石微粉钎焊后残余应力的分布状态,文中对不同形体的金刚石(球体、正十二面体和梯台体)进行有限元模拟,模拟出3种形状金刚石键合区残余应力分布,并用拉曼光谱实测3种形状金刚石粉末在钎焊后键合处的残余应力,验证所建模型的准确性.通过数值模拟结果可知,3种金刚石的残余应力从侧壁键合区和金属化合物键合区逐渐扩展至钎料和与钢基体内部,经剖面细节分析,梯台体金刚石的残余应力最大,正十二面体金刚石残余应力最小.基于拉曼光谱峰位移计算可知,3种形态金刚石均受拉应力,梯台体金刚石冷却后残余应力约为552.36 MPa,球体金刚石冷却后残余应力约413.19 MPa,正十二面体金刚石冷却后残余应力约为288.19 MPa,数值模拟计算值和实测值之间容差为3% ~ 25%.

     

    Abstract: Due to the irregular broken shape of fine-grained diamond powder and the large difference in linear expansion coefficients between the diamond and filler metal, residual stress is prone to occur at the interface of diamond tools during brazing, which seriously affects the machining performance of the tools. To analyze the residual stress distribution of diamond powder after brazing in detail, finite element simulations were conducted on diamonds with different shapes (spherical, regular dodecahedron, and trapezoidal body). The residual stress distributions in the bonding zones of these three diamond shapes were simulated. Meanwhile, the actual residual stresses at the bonding interfaces of the three diamond powder shapes after brazing were measured using Raman spectroscopy to verify the accuracy of the established model. The numerical simulation results indicate that the residual stress of the three types of diamonds extends gradually from the sidewall bonding zone and the intermetallic compound bonding zone to the interior of the filler metal and steel substrate. Through detailed cross-sectional analysis, the residual stress of the trapezoidal diamond is the largest, while that of the regular dodecahedron diamond is the smallest. Based on Raman spectral peak shift calculations, all three forms of diamonds are subjected to tensile stress. The residual stress of the trapezoidal diamond after cooling is approximately 552.36 MPa; that of the spherical diamond is approximately 413.19 MPa, and that of the regular dodecahedron diamond is approximately 288.19 MPa. The deviation between the numerical simulation values and the measured values ranges from 3% to 25%.

     

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