在DIL 805A膨胀仪上测定了Nb微合金化1000 MPa级冷轧双相钢连续加热及两相区保温过程中的热膨胀曲线,根据杠杆定律计算的奥氏体体积分数与定量金相测量值符合较好.740、770和800℃保温100 s的过程中,奥氏体的等温相变动力学曲线明显分为两个阶段,两个阶段可分别由JMAK方程描述.第Ⅰ阶段时间指数较大,奥氏体体积分数增长较快,奥氏体长大由C的扩散控制;第Ⅱ阶段时间指数降低,奥氏体体积分数的增长明显变慢,奥氏体长大转变为由Mn的扩散控制.在较低的保温温度下,奥氏体长大可以更快的由C扩散控制转变为由Mn扩散控制.
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