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首页> 外文期刊>Materials Science and Engineering >Dynamic mechanical behaviors and failure thresholds of ultra-high strength low-alloy steel under strain rate 0.001/s to 10~6/s
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Dynamic mechanical behaviors and failure thresholds of ultra-high strength low-alloy steel under strain rate 0.001/s to 10~6/s

机译:超高强度低合金钢在应变率0.001 / s至10〜6 / s下的动态力学行为和破坏阈值

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In this study, the dynamic mechanical behaviors of the typical ultra-high strength low-alloy martensite steel 35CrMnSiA under strain rate 0.001/s~106/s were studied through quasi-static compressive tests (0.001/s), SHPB tests (2000/s~5000/s) and planar plate impact tests together with DISAR tests (105/s~106/s). The XRD analysis and metallographic observation were conducted to investigate the microstructure evolutions and failure mechanism of 35CrMnSiA under different stress states. Under uniaxial stress state, the adiabatic shear failure occurs as long as the rise rate of plastic strain energy density reaches 10.58×106J·m−3µ s−1and the plastic strain energy density is above 4.51×108J·m−3. For 35CrMnSiA samples under uniaxial strain state, the critical pressure for reversible phase transformation (α→ε, BCC→HCP) falls in the range of 17.57–19.19 GPa. Characterized by prominent temperature rise and volume shrinkage, theα→εphase transformation induced by continuous dynamic recrystallization contributed to increasing the strength but weakening the ductility of 35CrMnSiA. In addition, the Hugoniot coefficients for 35CrMnSiA under a wide range of pressures have been determined. Moreover, the failure thresholds for 35CrMnSiA were obtained by dynamic fracture experiments and high velocity impact experiments: 35CrMnSiA projectiles fractured over impact pressure of 2.59 GPa, and when the impact pressure exceeded 21.25 GPa above which 35CrMnSiA suffered phase transformation, the projectiles had severe mass abrasion.
机译:通过准静态压缩试验(0.001 / s),SHPB试验(2000 / s),研究了典型超高强度低合金马氏体35CrMnSiA在应变率0.001 / s〜106 / s下的动态力学行为。 s〜5000 / s)和平板冲击试验以及DISAR试验(105 / s〜106 / s)。通过XRD分析和金相观察,研究了35CrMnSiA在不同应力状态下的组织演变和破坏机理。在单轴应力状态下,只要塑性应变能密度的上升率达到10.58×106J·m-3μs-1,且塑性应变能密度大于4.51×108J·m-3,就会发生绝热剪切破坏。对于单轴应变状态下的35CrMnSiA样品,可逆相变的临界压力(α→ε,BCC→HCP)在17.57–19.19 GPa范围内。连续动态再结晶引起的α→ε相变具有明显的温度升高和体积收缩的特征,有助于提高强度,但削弱了35CrMnSiA的延展性。另外,已经确定了在宽压力范围内35CrMnSiA的Hugoniot系数。此外,通过动态断裂实验和高速冲击实验获得了35CrMnSiA的破坏阈值:35CrMnSiA弹丸在2.59 GPa的冲击压力下破裂,当冲击压力超过21.25 GPa时,超过35CrMnSiA的相变,则弹丸具有严重的整体磨损。

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