通过分段淬火连续退火实验,获得两组铁素体晶粒尺寸大致相同、马氏体体积分数不同的双相钢.选取应变速率为10-4s-1进行准静态拉伸实验；选取应变速率为500s-1和2250s 1在分离式霍普金森拉杆技术进行动态拉伸实验.利用动态因子、Feret比率等定量分析方法研究超高强铁素体马氏体双相钢在动态拉伸变形条件下的组织和性能.结果表明:应变速率效应在双相钢的动态变形行为中主要起强化作用；马氏体体积分数越低的双相钢应变速率敏感性越大；相比抗拉强度而言,超高强冷轧双相钢屈服强度的应变速率敏感性更大.计算在应变速率为2250s1动态拉伸变形下产生绝热温升分别为98K和89K,并抵消部分应变速率强化作用.
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