共查询到18条相似文献,搜索用时 62 毫秒
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经强冷变形后的单晶铜线会产生明显的亚结构。在退火过程中该亚结构将发生转变.以中拉单晶铜线为对象,通过金相、力学性能测试法、电阻测试等手段研究了经强冷变形后的单晶铜线在不同退火工艺制度下的组织性能变化和再结晶过程.研究结果表明:加工态单晶铜线材的再结晶温度开始在250℃左右,比相同冷变形率下的SCR连铸纯铜杆的再结晶温度高约50℃.强冷变形单晶铜线再结晶形核的孕育期随温度升高而缩短.500。C时的孕育期不足2min.单晶铜在退火的回复阶段导电性能得到改善,但温度较高发生再结晶时,由于晶界数量的不断增加,有抑制电阻率减小的作用.强冷变形后的单晶铜线要想恢复足够的塑性,则难以避免成为多晶,如果既要恢复单晶铜线的塑性和导电性,又要维持单晶的组织形态,进行高温超短时间退火将有助于解决这一问题. 相似文献
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采用自制真空熔炼、氩气保护连续定向凝固设备成功制备出了大直径单晶纯铜棒材,研究了工艺参数对大直径连续定向凝固纯铜棒材凝固组织与表面质量的影响,分析测试了连续定向凝固大直径纯铜棒材的力学性能和电学性能.结果表明:在熔体温度1150~1180℃、结晶器出口温度750℃、冷却水量900 L·h-1、冷却距离50mm以及拉坯速度9mm·min-1时,可连续稳定地制备直径为φ16mm的表面光亮的单晶纯铜棒材.其抗拉强度128.52MPa,延伸率76.7%,导电率105.2%IACS,具有优良的力学性能和电学性能. 相似文献
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金属单晶和多晶电子通道花样的观察与分析孙丽虹,刘安生,张启海(北京有色金属研究总院100088)关键词:扫描电镜,电子通道花样,金属单晶与多晶1967年英国人Coates[1]首次用扫描电镜在硅、锗等单晶中观察到电子通道花样(ECP),开拓了扫描电镜... 相似文献
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对多晶铜线材拉拔变形后做成的标准样品的极图、取向分布函数(ODF)和反极图进行测定,研究和分析该材料的形变织构类型和分布情况,为产品的质量控制和工艺过程提供理论依据。 相似文献
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对Nb47Ti合金丝材进行了不同温度(750、800、850、900、950℃)的热处理,研究其微观组织结构、晶粒取向分布及性能的演变规律,结果表明:750℃×1 h/WQ热处理后的Nb47Ti合金具有最佳的强度与塑性匹配,其抗拉强度为586 MPa、断后伸长率为31.3%,断面收缩率为90.87%,维氏硬度为1 573 MPa;随着热处理温度升高,Nb47Ti合金晶粒呈长大的趋势,平均晶粒尺寸从29.3μm增加到89.8μm;热处理会明显改变Nb47Ti合金的取向差分布。 相似文献
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介绍了热型连铸技术的原理、优点、关键技术和工艺参数。重点介绍了热型连铸技术在单晶铜生产中的应用,提出了该技术存在的问题及今后的改进方向和发展趋势。 相似文献
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以纯度(质量分数)为99.95%的钨粉为原料,经冷等静压成形,1 800~2 300℃高温烧结制得钨烧坯,钨烧坯在1 250~1 500℃经过4道次轧制制得接近理论密度的钨板。采用电子背散射衍射(EBSD)分析退火过程中钨板织构的衍变过程,通过金相、维氏硬度和高温抗拉强度分析退火过程中钨板组织和性能的变化规律。结果表明,轧制态的钨板晶粒组织明显沿轧制方向拉长;1 150℃和1 250℃退火10 min后,织构类型没有发生明显变化,晶粒仍为拉长状态;1 350℃退火后,形变织构明显减弱,晶粒取向分布趋于随机。通过统计面积分数分析得到,1 350℃退火后钨板晶粒再结晶组织比例占65.8%。轧制钨板的显微硬度和高温抗拉强度随退火温度的升高而降低,1 150℃退火后的显微硬度和高温抗拉强度分别为430 HV和485 MPa,1 350℃退火后的显微硬度和高温抗拉强度分别为410 HV和356 MPa。 相似文献
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Recrystallization of Single Crystal Nickel-Based Superalloy 总被引:1,自引:0,他引:1
A series of experiments of investigating the recrystallization of single crystal DD3 superalloy were carried out. The threshold temperature for recrystallization and the effect of annealing temperature on recrystaUization were studied. The results show that the threshold temperature for recrystallization of the shot-peened DD3 samples is be-tween 1 000 ℃ and 1 050℃ under the condition of annealing for 2 h, and the recrystallization depth increases with the rise of the annealing temperature. Below 1 150 ℃, the recrystallization depth increases slowly with the tempera-ture climbing, while above 1 150 ℃, the recrystallization depth increases quickly with the rise of the temperature. The solution of the γ' phase is a critical factor of the recrystallization behavior of DD3 superalloy. In addition, the ki-netics and microstructural evolution of recrystallization at 1 200 ℃ were also studied. It is found that the recrystalli-zation progresses rapidly at 1 200℃ through the growth of fully developed recrystallized grains, and the recrystalli-zation process on the shot-peened surface is similar to that of wrought materials, including nucleation of reerystalliza-tion, growth of new grains into the matrix, and growth of new grains by swallowing up each other. 相似文献
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Recrystallization of a Single Crystal Nickel-Base Superalloy 总被引:2,自引:0,他引:2
A series of experiments of investigating the recrystallization of single crystal DD3 superalloy were carried out. The threshold temperature for recrystallization and the effect of annealing temperature on recrystallization were studied. The results show that the threshold temperature for recrystallization of the shot peened DD3 samples is between 1 000 ℃ and 1 050 ℃ under the condition of annealing for 2 h, and the recrystallization depth increases with the rise of the annealing temperature. Below 1 150 ℃, the recrystallization depth increases slowly with the temperature climbing, while above 1 150 ℃, the recrystallization depth increases quickly with the rise of the temperature. The solution of the γ′ phase is a critical factor of the recrystallization behavior of DD3 superalloy. In addition, the kinetics and microstructural evolution of recrystallization at 1 200 ℃ were also studied. It is found that the recrystallization progresses rapidly at 1 200 ℃ through the growth of fully developed recrystallized grains, and the recrystallization process on the shot peened surface is similar to that of wrought materials, including nucleation of recrystallization, growth of new grains into the matrix, and growth of new grains by swallowing up each other. 相似文献
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在配置Φ152mm坩埚的单晶炉内,合理地调整了温度分布场与控制条件,成功地拉制出一根Φ128~140mm,有效长度为12mm的N型锗单晶 相似文献
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基于国内某钢厂CSP漏斗结晶器铜板结构,建立了考虑铜板水槽冷却水流动的薄板坯结晶器铜板三维热/力耦合计算模型,研究分析了典型连铸工艺下结晶器铜板水槽内冷却水的传热特点和铜板温度场与热应力场分布规律,并探讨了冷却水流速及铜板厚度对铜板热/力行为的影响。结果表明,铜板宽面热面与窄面热面最高温度均位于弯月面下约15 mm处,分别达436.5、379.2 ℃。宽面和窄面铜板的最大热应力均位于弯月面下方约25 mm处,分别达876.7、867.8 MPa。宽面铜板的热应力总体比窄面高且分布更为不均匀,螺栓处热面的热应力整体低于其两侧水槽处热面的热应力。增加冷却水流速、减小铜板厚度可减小铜板热面温度与热应力。将螺栓处冷却水缝延长到距结晶器下口30 mm处,可显著改善宽面铜板中下部横向温度分布的均匀性,使其热面横向最大温差减少约19.6 ℃。 相似文献