压缩双裂纹和单裂纹圆孔板应力强度因子公式

从理论模型和数值分析上澄清了国外文献关于压缩双裂纹圆孔板(double cleavage drilled compression,DCDC) 的应力强度因子不同的公式引起的混淆. 证明Plaisted 等用修正压缩无限大板中圆孔双边裂纹的解和欧拉-伯努利梁理论得到的DCDC 应力强度因子公式都存在推导和原理性的失误. 指出Jenne 等推导的公式形式过于复杂不便使用, 而He 等的公式适用范围偏小. 通过拟合有限元法宽范围数值计算结果导出DCDC 的应力强度因子的新公式, 该公式形式简单, 对无量纲裂纹长度和无量纲板宽度适用范围较大, 最大误差是7%. 此外, 还对新提出的压缩单裂纹圆孔板(single cleavage drilled compression, SCDC)做了分析, 首次得到的SCDC应力强度因子公式的最大误差是5%. 给出的2 个公式可分别用于脆性材料DCDC 或SCDC 试样的断裂韧度测试.     

岩石偏心圆孔单裂纹平台圆盘的动态裂纹扩展与止裂

针对平台圆环构型的优点, 提出偏心圆孔单裂纹平台圆盘(cracked eccentrically holed flattened disc, CEHFD), 该试样具有更长的断裂路径。利用霍普金森压杆加载系统, 径向冲击CEHFD试样, 完成Ⅰ型动态断裂实验。砂岩试样表面粘贴应变片和裂纹扩展计, 用于监测裂纹动态起裂、扩展和止裂的全过程。实验表明, 在整个断裂过程中, 裂纹非匀速扩展, 裂纹扩展速度在裂纹起裂后加速上升, 在裂纹止裂前有明显的减速, 与地震时断层的动态破裂全过程完全吻合。采用实验-数值-解析法得到动态应力强度因子, 其时间历程呈现先增大后减小的趋势。根据断裂过程不同时刻, 得到相应的动态起裂韧度、扩展韧度及止裂韧度。在动态断裂全过程中, 动态扩展韧度为速度的函数, 变化趋势与速度一致, 随着时间先增大后减小; 动态起裂韧度大于动态止裂韧度, 止裂韧度随着裂纹最大扩展速度的增大而降低, 并且有较大的离散性。

     

用圆孔平台巴西圆盘确定岩石拉伸强度的非局部应力方法

对用圆孔平台巴西圆盘确定岩石拉伸强度的方法进行了研究.用有限元法分析了试件加载直径上的双向应力分布.由于加载直径靠近孔边处存在较大的拉伸应力梯度,如果以加载直径与中心圆孔相交点的最大拉伸应力来确定岩石的拉伸强度σt,拉伸强度的试验值会随着中心圆孔与圆盘半径之比r/R的增加而减小.采用非局部应力方法,考虑双向应力状态作用下发生破坏的Griffith强度准则的等效应力σG,在加载直径上选取材料特征尺寸,让σG"在特征尺寸上积分后取均值后得到岩石的拉伸强度σt.利用该方法得到的圆孔平台巴西圆盘测得的σt值不随r/R的变化而变化,其平均值大约为平台巴西圆盘测试值的1.23倍左右.     

中心直裂纹平台巴西圆盘复合型动态断裂实验研究

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。     

采用压缩单裂纹圆孔板确定岩石动态起裂、扩展和止裂韧度

爆炸、冲击、地震等人为或自然灾害不可避免,经常造成大量土木工程设施的破坏,因此岩石在动态载荷作用下的行为受到特别关注.岩石动态断裂韧度是评价岩石抵抗裂纹动态起裂、扩展和止裂性能的材料参数,开展岩石动态断裂韧度测试方法的研究对相关理论基础和实验技术的要求较高.岩石动态断裂韧度分为动态起裂、动态扩展、动态止裂三种,虽然关于动态起裂和动态扩展的研究已有一些成果,对岩石动态止裂的研究仍是一个难题,至今几乎无人问津.研究表明,在分离式霍普金森压杆撞击压缩单裂纹圆孔板岩石试样的I型动态断裂试验中,动态起裂、扩展、止裂的全过程可以由黏贴在压缩单裂纹圆孔板试样上的裂纹扩展计监测,岩石的动态起裂、扩展、止裂韧度可以用实验-数值-解析法确定.特别值得一提的是首次测出了岩石的动态止裂韧度.裂纹扩展计信号还显示,压缩单裂纹圆孔板在止裂后,停止的裂纹还会再次动态起裂、扩展并超出裂纹扩展计的检测范围.从能量的角度分析了动态止裂的过程,指出测试动态止裂韧度时要注意的一些问题.结果显示,岩石动态起裂韧度和动态扩展韧度分别随动态加载率和裂纹扩展速度的增大而增大,岩石动态起裂韧度略大于动态止裂韧度.      

大理岩动态劈裂拉伸断裂的实验研究

利用直径为100mm的Hopkinson压杆和薄圆形铝片作为波形整形器,用不同弹速径向冲击大理岩平台巴西圆盘来研究其动态拉伸强度.考虑了试样的尺寸大小及两个平台附近应力的时间不均匀性与空间不均匀性对实验结果的影响.分析了试样的最大应变率、破坏时间、破坏模式以及破坏过程中的载荷应变关系,得到了关于大理岩在高应变率下拉伸强度及弹性模量的一些结论.进一步又利用该装置径向冲击人字形切槽巴西圆盘试样,对试样的起裂时间进行了初步的研究,以便今后测试动态断裂韧度.     

预制裂缝宽度对HCFBD试件确定岩石断裂韧度的影响

为了考察人工预制裂缝宽度对确定岩石断裂韧度的影响,采用大理岩制作了含有不同预制裂缝宽度的中心圆孔裂缝平台巴西圆盘试件(hole-cracked flattened Brazilian disc, HCFBD),在RMT150B试验机上进行试验,对不同预制裂缝宽度圆盘的应力强度因子进行有限元计算,并对测试方法进行了研究。结果表明,采用将预制裂缝宽度视作零宽度裂缝方法确定的断裂韧度值偏低,给出了一种采用最小载荷和最大无量纲应力强度因子确定岩石断裂韧度的新方法,该方法能够消除预制裂缝宽度对圆盘试件测定岩石断裂韧度的影响。     

SHPB冲击加载下四种岩石的复合型动态断裂实验研究

分别用绿砂岩、黄砂岩、灰砂岩、大理岩制作了三种几何相似的(φ80mm、φ122mm、φ155mm)中心直裂纹平台巴西圆盘(CSTFBD)试样;利用分离式霍普金森压杆加载,进行了I型和I-II型复合动态断裂实验,并由实验结合有限元分析得到了四种岩石材料的I、II型动态断裂韧度KId、KIId。研究表明:动态断裂韧度均存在尺寸效应,试样尺寸对I-II型复合比和纯II型加载角均会产生影响,复合比随尺寸的增大而减小,大尺寸试样II型加载的加载角比小尺寸试样的小。同时,由于负值的T应力显著减小了裂纹的起裂角,用广义最大拉应力准则预测的起裂角更符合实验结果。     

加载角度对层理页岩裂纹扩展影响的实验研究

采用分离式霍普金森压杆（SHPB）系统对页岩进行冲击实验,研究层理角度对页岩动态断裂过程的影响,在裂尖设置裂纹扩展计,借助高速摄影和数字图像相关（DIC）技术对页岩中心切槽半圆盘弯曲（NSCB）试件断裂的全过程进行研究,得到了不同加载角度下页岩的动态起裂韧度、裂纹扩展速度、断裂过程中应变场和水平位移场的变化规律。实验发现:不同加载角度下,页岩的动态起裂韧度具有显著的各向异性,加载角度与动态起裂韧度呈正相关;加载角度对试样的裂纹扩展速度具有显著影响,与裂纹扩展速度呈负相关;当冲击速度较低时,切槽方向是裂纹扩展的优势方向,而当冲击速度较高时,试样会产生沿层理弱面的次生裂纹,次生裂纹对试样的断裂具有显著影响。     

Sound emission by a vortex ring passing through a circular hole in a large flat plate

Acoustic emission has been studied experimentally when a vortex ring passes through a circular hole in a large flat plate, along its normal axis. The speed of the vortex ring is made high enough for the sound emission to be detectable, but can be regarded as sufficiently low in comparison to the sound speed. Substantial monopole and quadrupole components are observed in the detected wave profiles. Translational motion of the vortex ring in the presence of the flat plate with a hole has been observed optically, and its relation with the sound emission is determined. In this case, the power law of the acoustic pressure amplitude of monopolar vortex sound versus the translation speed U of the vortex ring is first measured in detail and is found to be U^2.1–U^2.4. This means that experimentally determined powers for the monopole components in the two half-spaces also agree approximately with the corresponding values predicted by the theory of vortex sound.     

Investigation of the stress field of a near-surface circular hole

By observing experimentally obtained photoelastic fringe patterns and applying classical solutions for an infinite plate containing a circular hole under remote tension and the modified Hertz contact theory, a replaced superposition method is proposed. In this paper we use this method to investigate the state of stress around a near-surface circular hole in a semi-infinite plate under a concentrated load. The well-matched conditions between the reconstructed and experimental photoelastic fringe patterns indicate the applicability of the proposed method. This paper was presented, in part, at a symposium honoring Dr. Christian P. Burger, Novel Applications of Experimental Methods in Mechanicsheld at the 2003 SEM Annual Conference and Exposition on Experimental and Applied Mechanics, June 2–4, 2003, Charlotte, North Carolina.     

Reinforcement of a plate with a circular hole by an eccentric circular patch

We study the reinforcement of an infinite elastic plate with a circular hole by a larger eccentric circular patch completely covering the hole and rigidly adjusted to the plate along the entire boundary of itself. We assume that the plate and the patch are in a generalized plane stress state generated by the action of some given loads applied to the plate at infinity and on the boundary of the hole. We use the power series method combined with the conformal mapping method to find the Muskhelishvili complex potentials and study the stress state on the hole boundary and on the adhesion line. We consider several examples, study how the stresses depend on the geometric and elastic parameters, and compare the problem under study with the case of a plate with a circular hole without a patch. In scientific literature, numerous methods for reinforcing plates with holes, in particular, with circular holes, have been studied. In the monographs [1, 2], the problem of reinforcing the hole edges by stiffening ribs is solved. Methods for reinforcing a circular hole by using two-dimensional patches pasted to the entire plate surface are studied in [3, 4]. The case of a plate with a circular cut reinforced by a concentric circular patch adjusted to the plate along the boundary of itself or along some other circle was studied in [5, 6]. The reinforcement of an elliptic hole by a confocal elliptic patch was considered in [7].     

Initiation and growth characterization of corner cracks near circular hole

The finite element analysis of crack problems often incorporates the asymptotic character of the local solution into the formulation. Embedment of stress or strain singularities can impose serious restrictions on the outcome and inconsistencies in predicting crack and/or growth. These restrictions are discussed in connection with the problem of two diametrically opposite corner cracks near a circular hole subjected to remote uniform tension. Enforced in the numerical treatment is the 1/r character of the strain energy density function local to the corner crack border where r is the radial distance measured from the crack front. The tendency for the corner crack to become a through crack is predicted by assuming that each point of the crack border extends by an amount proportional to the strain energy density factor. The path would correspond to the loci of minimum strain energy density function. Numerical results are displayed graphically and discussed in connection with crack initiation and non-self-similar crack growth.