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摘要: 研究了冲击波极端条件下玻璃介质的细观结构破坏问题,指出在低于Hugoniot弹性极限的应力区内,按照细观结构损伤程度的不同,在受压玻璃介质中可以划分出两个区域,即压缩区和破坏区。以K9和ZF1玻璃为例,通过双层结构样品实验,确认了玻璃样品的表面效应(即表面原生微裂纹的扩展)是破坏区形成的第一位原因。其次,基于对破坏区内细观结构损伤和破坏特性的分析,进一步提出:由于玻璃内部散布的不均匀相与其基体介质之间的压缩率不同,冲击波压缩造成了众多的局域变形点,当表面裂纹扩展到不均匀相与基体的边界处,会出现裂纹扩展路径拐折或分叉,造成介质的分割甚至粉碎,这是破坏区生成的第二位原因。Abstract: Experimental measurements were conducted for the shock compressed glasses at the stresses below their Hugoniot elastic limit ( HEL ). It has been revealed that, in terms of the microstructure damage degree, there exist two different regions within the stressed samples: a compressed (without damage) and a fractured regions, respectively. Results of K9 and ZF1 glasses with double-layer structure sample demonstrate that the formation of the fracture region could be due to an activation and development of the primary microcracks on glass surface under shock wave compression, which is the first cause. Besides, due to the different compressibility between the matrix and the inhomogeneous phases distributed in the original glass body, numerous locally strained spots would be produced under shock wave compression. When the surface microcracks propagate to the strained spot boundaries, new cracks are generated, accompanying with crack turning and branching, which makes glass body further fracture of fragmentize.
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Key words:
- shock wave /
- glass /
- damage
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Rasorenov S V, Kanel G I, et al. High Pressure Research, 1991, 6: 225. Bless S J, Brar N S, Kanel G I, et al. J Am Ceram Soc, 1992, 75: 1002. Raiser G, Wise J L, Clifton R J, et al. J Appl Phys, 1994, 75: 3862. Bourne N K, Rosenberg Z, Field J E. J Appl Phys, 1995, 78: 3736. Clifton R J. Appl Mech Rev, 1993, 46: 540. 王礼立. 应力波基础. 北京: 国防工业出版社, 1985: 43.
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