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为探究循环冲击损伤后大理岩的静态断裂力学特征,基于有限差分(finite difference method,FDM)-离散元(discrete element method,DEM)耦合的建模技术构建了三维分离式霍普金森压杆(split Hopkinson pressure bar,SHPB)数值模型,其中杆件系统和岩石试件分别采用FLAC3D和PFC3D程序建模。利用该模型对中心直切槽半圆盘(NSCB)试样进行了恒定子弹速度下的循环冲击,随后对受损试样进行静态三点弯曲断裂实验。通过编写Fish程序,提取试样断裂面数据,对断裂面进行重构并定量计算表面粗糙度。通过与相关室内实验结果的对比分析,验证了本文数值分析的合理性与可靠性。模拟结果表明,随着循环冲击次数的增加,试样内部微裂纹、破碎颗粒均增加。连接力场分布混乱,部分力链发生断裂。力链的变化是试样力学性能劣化的根本原因。在静态三点弯曲断裂实验中,冲击5次后试样的静态断裂韧度较天然试样产生一定程度的降低。试样在静载过程中产生的微裂纹和碎块的数量随循环冲击次数的增加而增加,断裂面粗糙度随循环冲击次数的增加而增加。 相似文献
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中心直裂纹平台巴西圆盘复合型动态断裂实验研究 总被引:2,自引:0,他引:2
制作了中心直裂纹平台巴西圆盘(cracked straight through flattened Brazilian disc-CSTFBD)试样,利用分离式霍普金森压杆(split Hopkinson pressure bar-SHPB)加载,进行了岩石纯Ⅰ型和复合型(Ⅰ+Ⅱ型)动态断裂实验。由于加载角(载荷方向与裂纹线的夹角)在制作试样时已经通过裂纹线与试样平台的位置关系确定,因此在实验中可以方便而准确地实施加栽。比较了纯Ⅰ型加载和复合型加载下压杆上记录的入射波、反射波和透射波的波形。采用实验与数值相结合的方法,将实验得到的动态载荷输入有限元程序,得到了纯Ⅰ型试样的动态断裂韧度和复合型试样的两种动态应力强度因子的时间历程。计算了加载角为15°的试样应力强度因子的复合比(KI(t)/KⅡ(t)),此计算值与文献结果吻合较好,验证了实验方法的有效性。 相似文献
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E. N. Brown R. B. Willms G. T. Gray III P. J. Rae C. M. Cady K. S. Vecchio J. Flowers M. Y. Martinez 《Experimental Mechanics》2007,47(3):381-393
The current work presents the characterization and comparison of the mechanical response of three different industrial forms
of polyethylene. Specifically, high-density polyethylene (HDPE), ultra high molecular weight polyethylene (UHMWPE), and cross-linked
polyethylene (PEX) were tested in compression as a function of temperature (−75 to 100°C) and strain-rate (10−4 to 2,600 s−1). The responses of UHMWPE and PEX are very similar, whereas HDPE exhibits some differences. The HDPE samples display a significantly
higher yield stress followed by a flat flow behavior. Conversely UHMWPE and PEX both exhibit significant strain hardening
after yield. The temperature and strain-rate dependence are captured by simple linear and logarithmic fits over the full range
of conditions investigated. The yield behavior is presented in terms of an empirical mapping function that is extended to
analytically solve for the mapping constant. The power-law dependence on strain-rate observed in some polymers is explained
using this mapping function. 相似文献
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α-钛合金TA6的动态力学性能和剪切现象分析 总被引:1,自引:0,他引:1
诸多文献已经报道了β和(α β)钛合金冲击和爆炸加载下的绝热剪切现象,本文利用分离式的Hopkinson压杆和反射式Hopkinson拉杆对α-钛合金TA6的动态力学性能进行研究,得到不同应变率下材料的应力-应变曲线,发现钛合金TA6和其他钛合金一样也是一种应变率敏感材料。冲击拉伸加载时破坏形状45度剪切断口,然而其在冲击压缩应力作用下体现为典型的韧性,并未出现其它类型钛合金通常会出现的绝热剪切破坏。进一步分析表明:α-钛合金TA6不同于β和(α β)的钛合金,α-钛合金TA6相对于β和(α β)的钛合金是一种绝热剪切不敏感的材料。同时也利用应力状态的柔韧系数的概念对拉伸时45度的剪切断口解释。 相似文献
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A rigorous experimental and numerical assessment is made of the benefits and limits of miniaturization in the Kolsky bar system.
The primary issues that arise in very high strain rate testing (stress equilibration, inertial effects, wave dispersion, friction,
and controllability of deformations) are addressed through experiments coupled with explicit finite element analyses. A miniaturized
Kolsky bar system that includes the input bar is developed, together with the use of the laser occlusive radius detector to
obtain local measurements of specimen strain during the very high rate deformations. It is demonstrated that this miniaturized
Kolsky bar system can be used to provide fully validated results, including the explicit determination of equilibration, over
a very wide range of strain rates (1×103 to 5×104 s−1). The desired high strain rate can be achieved even at low accumulated strains, and the total strain developed can be controlled
very effectively. Specific conditions are developed for determining the range of utility of the technique for a given material.
The technique is applied to the characterization of 6061-T651 aluminum, and the results are compared with the results obtained
using a conventional Kolsky bar. 相似文献
9.
We conducted dynamic and quasi-static compression experiments with low-density (ρ = 120 kg/m3) epoxy foam specimens. The specimens had a 10.0-mm-square cross-section and a length of 19.3 mm. Dynamic experiments were
conducted with a modified split Hopkinson pressure bar (SHPB), and the quasi-static experiments were conducted with a hydraulic
load frame device (MTS-810). In both cases, the specimens were loaded from one end at a constant velocity. Equally spaced
grid lines were marked on the specimens to monitor the deformation history. Digital images taken at equally spaced time intervals
gave the positions of each grid line. These images showed that a constant end-face velocity V produced a compaction wave front that traveled at a constant velocity C in both dynamic and quasi-static experiments. We described these results with a shockwave analysis that used a locking solid
material model. 相似文献
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