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1.
李一凡  董世明  华文 《岩土力学》2016,37(11):3191-3196
为了研究中心裂纹巴西圆盘试件在压缩载荷作用下T应力的解析计算方法,通过权函数法推导出集中载荷作用下T应力的显式表达式,进而得到分布载荷作用下的T应力表达式。与边界配位法进行对比,所得公式优点在于任意相对裂纹长度和任意加载角下的T应力值都能较容易的精确得到。进一步分析表明,分布载荷与集中载荷作用下T应力的偏差随着载荷分布角的增加而增加。集中载荷作用下,相对裂纹长度固定时,T应力随着加载角的增大而增大。中心裂纹巴西圆盘纯I型与纯II型断裂试验时,大多数情况下的T应力都为负值。T应力值对中心裂纹巴西圆盘测定断裂韧度试验有影响,想要通过使T应力为0来消除这种影响是很难达到目的的。  相似文献   

2.
以CCD相机配合高速相机搭建试验变形观测系统,开展不同加载速率下含Ⅰ型预制裂纹花岗岩试件的三点弯试验。利用数字散斑相关方法对试验过程采集的数字散斑图像进行分析,对不同加载速率作用下含Ⅰ型预制裂纹花岗岩试件裂纹扩展过程中的变形演化特征、裂纹扩展速率、裂纹尖端张开位移、裂纹张开角以及初始断裂应力强度因子进行研究,研究结果表明:(1)花岗岩试件初始裂纹扩展速率随着加载速率的增加总体呈线性增加趋势;最大扩展速率随着加载速率增加呈现先较快增加后缓慢增加的变化趋势。(2)不同加载速率作用下,花岗岩试件预制裂纹尖端张开位移均呈现非线性缓慢增长-迅速增长-线性增长的变形趋势,且线性增长阶段曲线斜率随着加载速率的增加而增大。(3)随着加载速率的增加,花岗岩试件初始裂纹张开角先逐渐减小后稳定在0.1o~0.13o。(4)随着加载速率的增加,花岗岩试件初始断裂应力强度因子呈指数增长。  相似文献   

3.
李一凡  董世明  李念斌 《岩土力学》2016,37(Z1):645-650
平台巴西圆盘(CFBD)具有避免加载点处应力集中、保证破坏由预制裂纹尖端处起始的优点,成为研究脆性材料断裂性能的常用试件之一。最近的研究发现,T应力也会影响材料断裂性能,但平台巴西圆盘并没有计算T应力的解析公式。使用解析分析与有限元数值分析相结合的方法,对复合型加载条件下平台巴西圆盘试件的T应力进行了计算,并对误差进行了系统的分析。结果表明,在一定载荷分布角内相对裂纹长度 时,不管是纯I、纯II还是复合型加载条件下平台巴西圆盘计算的T应力都可以用中心裂纹巴西圆盘均布载荷下T应力计算公式来计算;T应力相对误差随着相对裂纹长度的增加而增加。  相似文献   

4.
徐积刚  董世明  华文 《岩土力学》2015,36(7):1959-1965
为了研究围压对巴西裂纹圆盘应力强度因子的影响,使用权函数方法得到了围压作用下巴西裂纹圆盘的应力强度因子,进而得到径向集中荷载与围压共同作用下的应力强度因子的计算公式。在此基础上,从理论上分析了围压对巴西裂纹圆盘应力强度因子的影响,分析结果表明:围压对II型应力强度因子无影响,纯围压作用下裂纹趋于闭合;围压和集中力共同作用下,I型应力强度因子随着围压的增大而减小。对比分析了数值分析与理论结果,分析表明,理论与数值结果吻合良好,从而表明了理论分析的正确性。此外,还研究了围压对纯II型裂纹加载条件的影响,结果表明,纯II型裂纹的临界加载角随着围压增大而减小,直至为0。因此,当围压较大时,加载角为0°左右所发生的断裂不一定全是纯I型断裂。  相似文献   

5.
华文  董世明  徐积刚 《岩土力学》2016,37(3):753-758
岩石断裂韧度表征其抵抗裂纹起裂和扩展的能力,作为其力学性能的一个重要指标,在岩石力学理论研究与岩体工程应用中有着不可替代的作用。由于岩石结构的复杂性,其破坏形式大多呈现为复合型断裂破坏,研究复合型加载条件下岩石断裂韧度具有重要的意义。为了研究锈岩的断裂力学性能,以便其在建筑工业中得到更为广泛的应用,通过18个中心裂纹圆盘(CSTBD)试件径向受压试验,进行了复合型加载条件下锈岩断裂韧度的试验研究。测得了锈岩在纯I型,纯II型以及复合型加载时的断裂韧度,并将试验结果与基于广义最大周向应力(GMTS)准则的理论值进行了对比分析,结果表明:锈岩的纯I型断裂韧度为1.01 MPa?m0.5,而纯II型断裂韧度为1.51 MPa?m0.5,是纯I型断裂韧度的1.49倍,这与基于GMTS准则的理论值1.34非常接近,而比基于最大周向应力(MTS)准则的理论值0.87大很多。裂纹尖端附近的T应力及断裂过程区裂纹尖端的临界距离rc对岩石类材料的开裂路径以及复合型断裂韧度都有较大的影响。考虑了T应力的广义最大周向应力(GMTS)准则能很好的预测试验结果。  相似文献   

6.
《岩土力学》2017,(1):214-220
研究了集中加载、加载板加载和平台加载3种不同加载方式对巴西圆盘的宏观力学行为、开裂过程以及材料的抗拉强度的影响。对于平台加载方式给出了不同平台加载角时抗拉强度的修正系数。在数值模拟中,采用了自主开发的连续-非连续方法,该方法将拉格朗日元、变形体离散元及虚拟裂纹模型耦合在一起,既可以很好地模拟弹性阶段的变形,又可以较好地模拟材料的真实开裂过程。研究发现,采用平台加载方式,有利于圆盘中心起裂,而采用集中加载和加载板加载方式,圆盘的加载部位容易发生剪破坏。在圆盘中心起裂时,集中加载方式的抗拉强度的数值解最接近于选取的抗拉强度,然后是加载板加载方式,最后是平台加载方式。无论对于哪种加载方式,在材料的抗拉强度较小时,圆盘易于中心起裂,否则圆盘的加载部位将发生剪破坏。圆盘中心起裂后,众多微裂纹汇聚成的裂纹带在垂直方向不断扩展,直至贯穿整个圆盘,同时伴有应力波产生并传播。  相似文献   

7.
利用颗粒流程序(PFC) 对直切槽式圆盘试样进行巴西试验模拟,分析了不同的裂隙倾角和裂隙长度对直切槽式圆盘试样裂纹扩展规律的影响。根据起裂位置的不同,主裂纹可分为从裂隙尖端萌生的Ⅰ型主裂纹和从裂隙尖端一定距离处萌生的Ⅱ型主裂纹;次生裂纹可分为从加载点附近萌生的Ⅰ型次生裂纹和从远离加载点的一侧萌生的Ⅱ型次生裂纹。当裂隙长度保持不变而增大裂隙倾角时,主裂纹从Ⅰ型过渡为Ⅱ型,次生裂纹则从Ⅰ型转变为Ⅰ型和Ⅱ型共存,最后又变为Ⅰ型。当裂隙角度保持不变而增大裂隙长度时,主裂纹保持不变,次生裂纹则由Ⅰ型逐渐过渡为Ⅰ型和Ⅱ型共存。另外,当径向应力达到峰值应力之后,试样内会有大量的微裂纹萌生、扩展,造成了圆盘试样的破坏。从力链和能量角度来看,巴西圆盘试样的破裂过程是试样内部拉应力集中产生的颗粒间黏结破裂以及应变能释放的过程。  相似文献   

8.
《岩土力学》2017,(8):2395-2401
从理论和数值两个方面进行分析,发现受径向集中力和围压作用的中心裂纹圆盘(CCBD)试件裂纹面接触会对II型应力强度因子产生较大的影响。通过理论研究,分析CCBD受集中力和围压作用裂纹面接触时圆盘内部的应力场,采用断裂力学权函数理论,推导得出在集中力和围压共同作用下,考虑裂纹面闭合时应力强度因子的解析解。然后,使用ANSYS软件建立了相应的数值模型计算应力强度因子,并与理论解和相关文献进行对比验证,证明了理论公式的正确性。无论裂纹张合与否,所提出的解析公式都能计算出不同裂纹长度、加载角、围压和摩擦系数的应力强度因子。最后,利用公式分析摩擦系数对应力强度因子的影响,结果表明:随着摩擦系数的增大,I型裂纹的应力强度因子不变,II型裂纹的应力强度因子随之显著减小;当加载角较大时,裂纹面产生更为复杂的二次裂纹,故压剪断裂测试的推荐加载角范围为30°~50°。  相似文献   

9.
开展不同加载速率条件下岩石变形场演化特征的试验研究,对岩石安全施工及岩石工程灾害预测预警等具有重要意义。通过不同加载速率下红砂岩单轴压缩试验,在以数字散斑相关方法分析试件变形场的基础上,对加载速率与岩石变形局部化演化特征、泊松比变化及能量积累和释放特征的对应关系进行分析。结果表明:随着加载速率的增加,岩石试件的峰值强度及脆性呈增加趋势。加载速率越大岩石试件的变形局部化启动应力越接近强度峰值,且变形局部化启动时对应的应力量值总体上呈增加的趋势。在不同量级加载速率下岩石试件泊松比量值差别明显,总体趋势表现为:在岩石试件变形局部化启动前,随着加载速率增加,岩石试件泊松比减小;在岩石试件变形局部化阶段,随着加载速率增加,岩石试件泊松比增大。在能量积累阶段,岩石试件最大变形能密度随加载速率增加而增大;在能量释放过程中,岩石试件能量释放速率随着加载速率增加而增大。  相似文献   

10.
黄达  岑夺丰  黄润秋 《岩土力学》2013,34(2):535-545
加载速率对裂隙岩体的力学性质及变形破坏均有重要影响。利用二维颗粒流程序PFC2D开展了不同倾角非贯通单裂隙砂岩试件的单轴压缩试验,研究了中等应变率对裂隙砂岩应力-应变曲线特征、裂隙尖端应力状态、特征应力状态、岩体损伤及裂隙扩展等力学响应的影响规律。裂隙岩体应力-应变曲线呈现明显的波动性,定义应力突变指标 对应力突变型波动剧烈程度进行了定量统计分析:随应变率的增加,曲线应力突变波动越剧烈,且峰后明显大于峰前;随裂隙倾角的增大,波动幅度峰前增大,而峰后减小。裂隙尖端破裂应力随应变率增大均有所提高,随裂隙倾角的增大,切向剪应力 总体上呈增加变化,而法向应力 明显减小。尖端破裂时岩样加载应力 、岩样临界扩容应力 及峰值应力 均随应变率增大而增大。裂隙尖端的破裂可立即引起岩体扩容,一般应变率越低,岩体裂隙尖端破裂点 和扩容点 越接近峰值强度 。随着应变率的提高,损伤裂纹及宏观裂隙类型越多,岩体试件损伤破裂程度越强,特别是试件端部效应愈显著。裂隙首先以I型翼裂纹在其尖端起裂,而I型翼裂纹的扩展长度与加载速率与裂隙倾角具有较强的相关性。  相似文献   

11.
基于P-CCNBD试样的岩石动态断裂韧度测试方法   总被引:2,自引:0,他引:2  
苟小平  杨井瑞  王启智 《岩土力学》2013,34(9):2449-2459
预裂的人字形切槽巴西圆盘(Pre-cracked chevron notched Brazilian disc,简称P-CCNBD)是将人字形切槽巴西圆盘(cracked chevron notched Brazilian disc,简称CCNBD)的切槽尖端再稍加切削制成直裂纹前沿的试样。利用霍普金森压杆对P-CCNBD砂岩试样进行径向冲击,完成I型动态断裂试验后再做数值分析得到岩石的动态断裂韧度。为了验证数值模拟的可靠性,先进行了无限平面中一条有限尺寸裂纹表面受冲击拉伸作用的动态有限元分析,结果表明,数值模拟的结果与Shi得到的结果非常吻合。将试验-数值法和他人的准静态法分别确定的砂岩的动态起裂韧度进行对比,两种方法得到的结果有一定的差异。采用试验-数值法,将比较成熟的直裂纹巴西圆盘(cracked straight-through Brazilian disc,简称CSTBD)和P-CCNBD两种试样测得的结果进行对比,两者吻合较好。得到的动态起裂韧度都有随着加载率的增加而增大的加载率效应。分析了准静态法的缺陷,认为试验-数值法得到的结果更为合理。  相似文献   

12.
The cracked chevron notched Brazilian disc (CCNBD) specimen has been suggested by International Society for Rock Mechanics for measuring mode I fracture toughness of rocks. Subsequently, this specimen geometry has been widely extended to conduct mixed mode fracture tests on rocks as well. A straight through crack front during the fracturing process upon the root of the chevron notch is assumed in the testing principle, but has never been thoroughly evaluated before. In this study, for the first time, the progressive rock fracture mechanism of the CCNBD rock specimen under mixed mode loading is numerically simulated. Specimens under representative mixed mode loading angles are modelled; and the assumption of the straight through crack front growth is critically assessed. The results show that not only the notch tip but also the saw-cut chevron notch cracks during the experiments, yielding a prominent twisted front, far from being straight. The crack front never grows up to the root of the notch ligament and the straight through crack front assumption is never satisfied in the realistic rock fracture progress of this chevron notched specimen subjected to mixed mode loads. In contrast, the fracture progress features typical three-dimensional wing cracking towards the loading ends. The numerically observed progressive fracture mechanism reveals that the measuring principle of mixed mode fracture tests employing CCNBD specimens is significantly violated and the measures of both modes I and II fracture toughness are uncertain.  相似文献   

13.
The cracked chevron notched semi-circular bending (CCNSCB) method falls into a significant testing category of chevron notched specimens for measuring the mode I fracture toughness, of which the progressive fracture mechanism deserves to be further assessed under intermediate dynamic loading rate (IDLR). In this study, the discrete element method (DEM) is adopted to depict the three-dimensional fracture processes of the CCNSCB specimens subjected to different IDLRs considering different supporting spans. The results demonstrate that the crack front of the CCNSCB specimen with any loading condition is prominently curved, which violates the straight-through crack propagation assumption and may induce some errors in the fracture toughness measurements. For each IDLR, the peak force of the CCNSCB specimen evidently increases with decreased supporting span, and the effect of loading rate on this parameter is more prominent for a smaller supporting span. For a relatively large span, the crack grows restrictively in the notched ligament, which conforms to the ideal assumption of the fracture process and contributes to an accurate measurement of the mode I fracture toughness. Thus, a large supporting span is suggested for the semi-circular bend tests. Additionally, the critical crack length and peak force are found dependent on the loading rate, and they are larger for the higher loading rate. Thus, the critical crack length determined under quasi-static conditions is not strictly suitable for the specimens under different IDLRs, especially for the much higher IDLR. This study calls for more attention on how to accurately determine the fracture toughness via chevron notched samples.  相似文献   

14.
Mixed mode fracture experiments were conducted on Harsin marble using two disc-shape samples namely the Brazilian disc (BD) and the semi-circular bend (SCB) specimens. For each specimen, a complete fracture toughness envelope ranging from pure mode I to pure mode II was obtained. The experimental results indicate that the mixed mode fracture toughness depends on the geometry and loading conditions such that for any similar mode mixture, the BD test data were significantly greater than the SCB fracture toughness results. Therefore, the conventional fracture criteria which present a unique mixed mode fracture curve, fail to predict the test results. It is shown that a generalized criterion, which takes into account the effects of geometry and loading conditions, is able to provide individual fracture curves for theses specimens with very good estimates for the test results obtained from both BD and SCB specimens. The BD and SCB specimens can be suggested as appropriate specimens for obtaining typical upper bound and lower bound envelopes for mixed mode fracture toughness of rocks.  相似文献   

15.
Numerical and experimental studies were performed on a new fracture test configuration called the edge cracked triangular (ECT) specimen. Using several finite-element analyses, the fracture parameters (i.e., K I, K II, and T-stress) were obtained for different combinations of modes I and II. The finite-element results show that the ECT specimen is able to provide pure mode I, pure mode II, and any mixed-mode loading conditions in between. Also, a series of mixed-mode fracture experiments were conducted on Neiriz marble rock using the proposed specimen. Furthermore, the generalized maximum tangential stress (GMTS) criterion was used to predict the experimental results. The GMTS criterion makes use of a three-parameter model (based on K I, K II, and T) for describing the crack tip stresses. Due to the significant positive T-stresses that exist in the ECT specimen, typical minimum fracture toughness values were expected to be obtained when the ECT specimen is used. The direction of fracture initiation and the path of fracture growth were also obtained theoretically using the GMTS criterion, and good agreement was observed between the experimental fracture path and theoretical simulations. The fracture study of this specimen reveals that the ECT specimen can be also used in mixed-mode fracture studies of rock materials in addition to the conventional circular or rectangular beam test samples.  相似文献   

16.
Indirect tension tests using Brisbane tuff Brazilian disc specimens under standard Brazilian jaws and various loading arcs were performed. The standard Brazilian indirect tensile tests caused catastrophic, crushing failure of the disc specimens, rather than the expected tensile splitting failure initiated by a central crack. This led to an investigation of the fracturing of Brazilian disc specimens and the existing indirect tensile Brazilian test using steel loading arcs with different angles. The results showed that the ultimate failure load increased with increasing loading arc angles. With no international standard for determining indirect tensile strength of rocks under diametral load, numerical modelling and analytical solutions were undertaken. Numerical simulations using RFPA2D software were conducted with a heterogeneous material model. The results predicted tensile stress in the discs and visually reproduced the progressive fracture process. It was concluded that standard Brazilian jaws cause catastrophic, crushing failure of the disc specimens instead of producing a central splitting crack. The experimental and numerical results showed that 20° and 30° loading arcs result in diametral splitting fractures starting at the disc centre. Moreover, intrinsic material properties (e.g. fracture toughness) may be used to propose the best loading configuration to determine the indirect tensile strength of rocks. Here, by using numerical outcomes and empirical relationships between fracture toughness and tensile strength, the best loading geometry to obtain the most accurate indirect tensile strength of rocks was the 2α?=?30° loading arc.  相似文献   

17.
Summary The effect of testing method and specimen geometry such as diameter, thickness, and crack length and type on measured fracture toughness was investigated using specimens collected from a limestone rock formation outcropping in the Central Province of Saudi Arabia. Straight Edge Cracked Round Bar Bend (SECRBB), semicircular disk specimens under three point bending, and Brazilian disk specimens under diametrical compression were used in this investigation. SECRBB specimens were used for the Mode-I study, and notched Brazilian disk and semicircular specimens were used for the mixed Mode I–II study. The results show that specimen diameter and crack type have a substantial influence on the measured fracture toughness; however, loading rate, crack size, and specimen thickness seem to have a negligible effect on the fracture toughness. Mode-I fracture toughness is significantly influenced by specimen diameter and crack type, while their effects on Mode-II fracture toughness are generally negligible. The different specimens (SECRBB, Brazilian disk, and semicircular) can give comparable results only when the proper span to diameter ratio is used. The Brazilian disk with a straight notch was found to be the most convenient geometry to use for fracture toughness determination. A simple method of making a precise notch inside the disk is presented, using the combination of a drilling machine and a wire saw.  相似文献   

18.
动载确定方法对岩石动态断裂韧度测试的影响   总被引:1,自引:0,他引:1  
张盛  李新文  杨向浩 《岩土力学》2013,34(9):2721-2726
为了考察不同方法确定的动态载荷对测试岩石动态断裂韧度的影响,在SHPB压杆系统上动态冲击直径80 mm的大理岩圆孔裂缝平台巴西圆盘,获得了弹性压杆上的应力波形,间接计算得到3种不同的作用在圆盘端部的动态载荷。将载荷输入ANSYS动态有限元模型中,求得了相应的动态应力强度因子,并根据试验-数值分析方法确定了岩石的动态断裂韧度测试值。结果表明,在加载速率约为4.0×104 MPa•m1/2/s的条件下,采用三波法确定的大理岩的平均动态断裂韧度为 3.92 MPa•m1/2,采用一波法比三波法计算的结果偏低11.22%,采用二波法比三波法计算的结果偏高20.15%,3种方法得到的结果差异较大。应力波在传播过程中,通过圆盘表面和预制裂缝面发生散射,部分能量不断发生释放是造成圆盘试件两端加载载荷不相等的主要原因。三波法是3种方法中比较理想的动态载荷确定方法,但需要考察试件的动态应力平衡性。  相似文献   

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