摘要:
高熵合金(HEA)因其优异的机械性能和能量吸收能力,成为抗冲击载荷响应的重要材料。本文通过分子动力学模拟,系统探讨了Al0.3CoCrFeNi HEA板在单次及二次冲击载荷下的动态响应行为,揭示了其相结构演变、位错分布、能量吸收及多次冲击累积效应的规律。结果显示,首次冲击下,HEA板的塑性区域相结构演变与能量吸收方式具有显著的速度依赖性。在低速冲击下,能量主要通过位错网络进行吸收;在中速冲击下,位错与无序化原子共同吸收能量;在高速冲击下,无序化原子主导能量吸收。位错线长度在0.5-0.8 km/s内遵循线性增长方程l=3162.8v1-1239.9,而在更高速度下,受板厚度限制,位错线长度出现下降趋势。应力分析表明,冲击速度增加时,最大应力与速度呈二次关系:σ1=-14.48v1+114.04v12+29.02,而塑性区域边界应力与速度的关系为σ2=2.81v1-0.42v12+9.44。二次冲击下,几何特征方面,HEA板在冲击后形成类梯形的破坏区域,其上坑半径与冲击速度的关系为r=3.29v1-0.45v12+2.67,二次冲击的最小影响区域为L=-0.45(v12+v22)+3.29(v1+v2)+2×h×cot(θ)+5.34;抗冲击性能方面,随着首次冲击速度的增加,二次冲击后的剩余速度增大,材料抵抗能力降低,在距冲击中心10 nm处,弹道极限与首次冲击的关系为vbl=-8.6ev1/769+1383.6,然而,二次冲击速度的增加会使首次冲击的影响减弱。本研究为优化靶板在多次冲击条件下的设计优化提供了理论依据。
Abstract:
High entropy alloy (HEA) has become an important material for impact load response due to its excellent mechanical properties and energy absorption capacity. In this paper, the dynamic response behavior of Al0.3CoCrFeNi HEA plate under single and secondary impact loads was systematically discussed by molecular dynamics simulation, and the evolution of phase structure, dislocation distribution, energy absorption and cumulative effect of multiple impacts were revealed. The results show that under the first impact, the phase structure evolution and energy absorption mode of the plastic region of HEA plate exhibits significant velocity dependence. Under low velocity impact, energy is mainly absorbed by dislocation network; at medium velocity impact, both dislocations and disordered atoms contribute; under high velocity impact, disordered atoms dominate energy absorption. The length of dislocation lines follows a linear evolution equation of l=3162.8v1-1239.9 within the range of 0.5-0.8 km/s, while at higher velocities, dislocation line length decreases due to thickness limitations of the plate. Stress distribution analysis shows that the maximum stress has a quadratic relationship with velocity: σ1=-14.48v1+114.04v12+29.02, while the relationship between the boundary stress and the velocity in the plastic zone is σ2=2.81v1-0.42v12+9.44. In the context of the second impact, the geometric characteristics indicate that the HEA plate forms a trapezoidal damage region, with a relationship between the radius of the upper pit to the impact velocity expressed as r=3.29v1-0.45v12+2.67. Consequently, the minimum affected area from the second impact can be represented as L=-0.45(v12+v22)+3.29(v1+v2)+2×h×cot(θ)+5.34. In terms of impact resistance, an increase in the initial impact velocity leads to a greater residual velocity after the second impact, indicating a reduction in the resistance. At a distance of 10 nm from the impact center, the relationship between the ballistic limit and the first impact is vbl=-8.6ev1/769+1383.6. However, an increase in the second impact velocity gradually diminishes the effects of the first impact. This study provides a theoretical foundation for the optimization of target plate designs under multiple impact conditions.