摘要:
为探究反射爆炸应力波作用下动静裂纹贯通机理,本文采用动光弹的实验方法,研究了反射爆炸应力波作用下的动静裂纹作用关系及贯通后的瞬态卸荷现象产生机制。研究结果表明:P波的反射波PrP波前沿为拉伸波,后沿为压缩波,PrP拉伸波向裂纹尖端施加拉伸应力,增加动态强度因子,促进裂纹的扩展,而PrP波后沿压缩波向裂纹尖端施加压缩应力,降低动态应力强度因子,抑制裂纹的扩展。P波的反射波PrS波会导致裂纹扩展方向的偏转和速度的变化,呈现波浪状不稳定扩展。爆炸裂纹与静止裂纹贯通后,裂纹面附近储存的弹性能以卸载波的形式向外快速释放,卸载波在静止裂纹尖端出现应力集中,诱发了静止裂纹尖端次生裂纹的产生。
Abstract:
Using dynamic photoelastic experimental method, the effect of reflected explosive stress waves on dynamic cracks and the penetration of dynamic crack propagation in specimens containing cracks are studied. The full-field photoelastic fringe series of horizontal explosion cracks generated by cutting explosives in specimens containing cracks were recorded by a high-speed camera. From the initiation of the explosion to the penetration of the crack, there are three stages in total: Firstly, the explosion from the cutting explosive generates the crack and the incident blast stress wave propagated and acted on pre-existing vertical crack; Secondly, the reflected blast stress wave interacted with the crack; Thirdly, the propagating crack penetrated to the pre-existing crack and released unloading stress waves. By comprehensively considering the singular and non-singular stresses at the near- crack-tip region, three constant stresses controlled by the far field were adopted. Newton-Raphson iteration method was applied to analyze and calculate the stress intensity of mixed modes in dynamic crack initiation under the reflected stress wave loading. The results show that the leading wave of the reflected pressure wave (PrP) is a tensile wave, while the trailing wave is a compressive wave. The tensile wave of PrP applies tensile stress to the crack tip, increasing the dynamic intensity factor and promoting crack propagation. Conversely, the compressive wave of PrP applies compressive stress to the crack tip, reducing the dynamic stress intensity factor and inhibiting crack propagation. The reflected shear wave (PrS) causes unstable propagation of cracks, including changes in direction and velocity, resulting in a wavy outward expansion of the cracks. After the dynamic crack penetrated to the pre-existing crack, the stored elastic energy near the crack is rapidly released in the form of unloading waves. Stress concentration occurs at the tip of the stationary crack due to the unloading wave, inducing the generation of secondary cracks in the pre-existing crack.