Fe-C-Mn系冷轧双相钢两相区奥氏体化过程模拟

在对双相钢两相区奥氏体化过程进行热力学与动力学分析的基础上,建立了两相区奥氏体化过程的扩散模型,并采用显式有限体积法对740℃与780℃下的奥氏体化过程进行了数值求解.模拟结果表明:奥氏体长大初期受C元素在奥氏体中的扩散控制并很快达到亚平衡.该阶段奥氏体长大速度较快.奥氏体长大后期受Mn元素在铁素体中的扩散控制.该过程由于Mn元素的扩散速率比C元素的扩散速率低几个数量级而持续数千秒.当Mn元素在两相中的扩散通量相等时,奥氏体停止长大,Mn元素继续从铁素体向奥氏体中转移以完成其在两相中的均化.     

碳化物增强钢基复合材料的奥氏体化行为

研究了碳化钨（ＷＣ）增强钢基复合材料在９８０～１２４０℃温度范围的高温奥氏体化行为及相应的淬火硬化效应．发现此材料的奥氏体化温度范围宽,在９８０～１１００℃加热淬火均能得到细小的组织结构,而且具有显著的淬火硬化效果（ＨＲＣ６８）．并且测量及探讨了不同状态下大块硬质相、ＷＣ聚集区及基体显微硬度（ＨＶ０．０５）的变化以及与宏观洛氏硬度之间的关系．     

Effect of continuous annealing parameters on the mechanical properties and microstructures of a cold rolled dual phase steel

A cold rolled dual phase (DP) steel with the C-Si-Mn alloy system was trial-produced in the laboratory, utilizing a Gleeble-3800 thermal simulator. The effects of continuous annealing parameters on the mechanical properties and microstructures of the DP steel were investigated by mechanical testing and microstructure observation. The results show that soaking between 760 and 820℃ for more than 80 s, rapid cooling at the rate of more than 30℃/s from the quenching temperature between 620 and 680℃, and overaging lower than 300℃ are beneficial for the mechanical properties of DP steels. An appropriate proportion of the two phases is one of the key factors for the favorable properties of DP steels. If the volume fraction of martensite and, thereby, free dislocations are deficient, the tensile strength and n value of DP steels will decrease, whereas, the yield strength will increase. But if the volume fraction of martensite is excessive to make it become a dominant phase, the yield and tensile strength will increase, whereas, the elongation will decrease obviously. When rapid cooling rate is not fast enough, pearlite or cementite will appear, which will degrade the mechanical properties. Even though martensite is sufficient, if it is decomposed in high temperature tempering, the properties will he unsatisfied.     

X12CrMoWVNbN10-1-1铁素体耐热钢中的马氏体相变过程

通过膨胀试验研究了X12CrMoWVNbN10-1-1铁素体耐热钢在不同奥氏体化条件下的马氏体相变过程.结果表明:在温度1010~1 200℃奥氏体化15 min条件下,马氏体相变的开始温度点Ms与结束温度点Mf随着奥氏体化温度的增加而升高;在1070℃奥氏体化时,Mf随奥氏体化时间的延长而升高,而在奥氏体化时间小于3 h时,随着奥氏体化时间的增加,Ms上升,在奥氏体化时间超过3 h后,Ms稳定在460℃左右;根据膨胀曲线拟合得到在1070℃奥氏体化保温不同时间条件下的马氏体相变动力学方程.