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1.
水饱和裂纹对地壳岩样中地震波速及各向异性的影响   总被引:11,自引:3,他引:8       下载免费PDF全文
选择4种地壳岩石样品,经干燥或水饱和处理后在不同围压条件下测量了在其中传播的纵、横波的速度及其各向异性.在大气压条件下低孔隙度(<1%岩样中,水饱和样品中的纵波速度明显地比干燥样品中的高,但横波速度的差别不大.因为在低孔隙度岩样中纵波速度对孔隙流体的反应比横波速度敏感,可以用泊松比的变化来反映随着围压的增加晶粒间流体对弹性波传播特性的影响.根据实验数据,按O’Connell模型分别计算了干燥和水饱和岩样中的裂纹密度,与通过实测体应变曲线得到的裂纹孔隙度十分吻合.利用横波的速度和偏振特性可以推断岩样中定向排列微裂纹的空间取向情况.研究表明,同时测量在岩样中传播的纵、横波的速度,通过Vp/Vs比值可以给出有关颗粒边界流体的证据,也可以估计岩样中的裂纹密度.  相似文献   

2.
为了研究含气地层对地震波传播的影响,在地层温压条件下,用超声波测试了长庆油田苏里格气田砂岩样品在不同饱和度下的纵、横波速度和衰减Q值.实验表明砂岩样品的物性和流体含量对纵波的速度和衰减的影响均大于横波,含气饱和度大于60%时纵波Q值变化明显;物性越好,含气饱和度越高,纵波Q值越小,吸收越大.分析实验结果和相应的影响机理,给出了利用纵波的吸收衰减预测砂岩含气性的应用实例.  相似文献   

3.
为研究致密砂岩储层弹性波速度各向异性及弹性参数随围压的变化规律,应用地质力学研究所从美国New England Reaearch Inc引进的Autolab2000岩石物性实验设备,对采自长庆油田延长组储层的3组典型致密砂岩,对其X、Y、Z三个方向分别取样,进行了不同孔隙介质(干燥、饱水及饱油)条件下弹性波速度随围压(5~180 MPa)变化规律的实验研究工作,得到了X、Y、Z三个方向分别在干燥、饱水及饱油时的弹性波速度,并对X、Y、Z三个方向的各向异性进行计算和对比分析.同时根据测得的弹性波平均速度得到样品的弹性参数随围压的变化规律,对实验曲线进行拟合,获得不同孔隙介质条件下弹性波速度、各向异性、弹性参数随围压的变化规律及其拟合公式.结果表明,垂直方向速度值最低,横波各向异性指数小于纵波各向异性指数;随着围压的增加,致密砂岩波速增大,其各向异性以幂函数形式减小,体模量、弹性模量、剪切模量和拉梅常数以对数函数形式有不同程度的增加,泊松比因所含介质不同而有不同的变化趋势,除个别线外,拟合系数皆在0.956以上.在围压高于140 MPa时,干燥、饱水和饱油状态下的泊松比皆在0.24左右.  相似文献   

4.
刘斌 Kern  H 《地球物理学报》1998,41(3):371-381
在实验室中研究了蛇纹岩和角闪岩样品在不同温压条件下的纵、横波速度和Q值.这两种岩样对应的主要组成矿物叶蛇纹石和普通角闪石都具有很强的晶格优选方位(LPO).随着围压的增加,波速和Q值均增大,但是在相互正交的三个方向上(垂直或平行于层理面及线理方向)增大的速度并不相同,这与微裂隙的逐渐闭合密切相关.在600MPa的围压下升高温度直到600℃以上,由于微裂隙的热扩张受到约束,波速和Q值下降幅度很小.观测到的波速和Q值的各向异性具有不同的机理,波速各向异性主要与定向分布的微裂隙和主要矿物的LPO等构造因素有关;高围压下纵波Q值各向异性与速度各向异性正好相反,可能是由于形成层理面的定向排列的平板状矿物晶体沿不同方向边界之间接触程度不同造成的.  相似文献   

5.
为研究致密砂岩声波速度及其各向异性随围压的变化规律以及不同流体饱和状态下的弹性各向异性特征,钻取了不同方向的岩心并在实验室超声波频率下对致密砂岩的声学特性进行了测量,分别给出干燥和饱和水状态下,不同方向样品纵横波速度、刚性系数以及各向异性系数随围压的变化规律,并对实验结果进行了分析讨论.实验结果表明致密砂岩纵横波速度、纵横波速度比以及刚性系数均随围压增加而增加,但其在不同饱和状态下的变化率却截然不同;纵横波速度比、各向异性系数在饱和水状态下变化规律不明显,表明孔隙流体的存在对于岩石物理性质有着非常重要的影响.这方面的实验工作不但对于考察不同流体性质对致密岩石弹性各向异性影响是必要的,而且有助于致密砂岩油水和气层的识别.  相似文献   

6.
面向超深碳酸盐岩油气勘探开发中储层精细地震刻画问题,研发了高温(200℃)、高压(200 MPa)岩石弹性性质超声测量系统.收集塔里木盆地9块奥陶系超深碳酸岩储层岩石样品,通过高温高压条件下超声纵、横波速度测量发现,在围压保持69.0 MPa不变的情况下,当温度从25℃上升到200℃时,干岩石样品的纵、横波速度以及体积模量与剪切模量随着温度的升高而下降,纵波速度与体积模量最大降幅分别达到3.54%和7.54%,横波速度与剪切模量最大降幅分别达到4.57%和8.93%;在温度保持200℃不变情况下,当围压从69.0 MPa上升到137.9 MPa时,干岩石样品的纵、横波速度以及体积模量与剪切模量随着围压的升高而升高,纵波速度与体积模量最大升幅分别达到1.78%和3.39%,横波速度与剪切模量最大升幅分别达到1.95%和5.26%.在超深碳酸盐岩油气储层环境下,温度对碳酸盐岩岩石骨架弹性性质的影响可能超过围压对岩石骨架弹性性质的影响.岩石样品温度与围压循环实验表明,干岩石弹性性质与温度以及围压的变化关系不具可逆性,碳酸盐岩岩石样品弹性模量与温度之间总体上存在线性关系,其截距与斜率由碳酸盐岩...  相似文献   

7.
岩石的地震波速度是浅部地层地下识别和区域构造研究的基础.哈密地区是我国重要的产油区域之一.本文利用Autolab2000岩石物性测试仪器,研究了0~200 MPa(约0~7000 m地下深度)下干燥、饱油与饱水三种状态时的砂岩地震波速度,得到了四组砂岩样品在三种状态下的纵横波速度与压力的拟合关系式.实验发现:在三种不同状态下,砂岩样品的纵横波速度都与压力呈对数关系;对于纵波,干燥下的波速明显小于饱油与饱水,但是饱油与饱水两种状态下岩石的纵波速度差异很小,饱水时的纵波速度略大于饱油;对于横波,低压下三种状态的地震波速度基本没有差异,在高压下,饱油与饱水样品的横波速度明显小于干燥样品.  相似文献   

8.
利用Autolab 2000岩石物性测试设备,在0~200 MPa及三种不同孔隙流体条件下(干燥、水饱和及油饱和)研究了三种来自延长油田延长组的砂岩沿平行和垂直层面两个方向(即H和V)的纵波、横波速度,并分别计算了这些弹性波速的各向异性系数.结果表明:三种砂岩Y1、Y2和Y3两个方向上的VP、VSH和VSV均随围压增加而基本呈对数函数形式变化,且纵波饱油曲线的斜率远大于饱水;Y1、Y2砂岩H方向的VP、VSH和VSV在干燥、饱水和饱油条件下基本上均大于对应的V方向的波速;干燥、饱水和饱油条件下Y1、Y2的波速各向异性系数ε、γ和ζ和围压之间呈指数或二次函数降低;Y1、Y2、Y3三个岩样之间的速度各向异性差异明显,以Y2的各向异性最显著,其次是Y1,而Y3基本没有各向异性.另外,Y1、Y2的各向异性系数ε、γ和ζ之间表现出明显的与压力和流体状态相关性,且在实验压力范围内,饱油条件下的ε、γ均大于对应的饱水条件.实验结果可以为该地区地震资料的解释、油水层划分及与声波测井之间的对比提供重要的基础数据.  相似文献   

9.
含流体砂岩地震波频散实验研究   总被引:1,自引:0,他引:1       下载免费PDF全文
为了研究孔隙流体对不同渗透率岩石地震波速度的影响,在实验室利用跨频带岩石弹性参数测试系统得到了应变幅值10-6的2~2000Hz频段下的地震波速度和1 MHz频率下的超声波速度,利用差分共振声谱法得到了频率600Hz岩石干燥和完全饱水情况下岩石声学参数.实验表明,在低饱和度下,致密砂岩在地震和超声频段下没有明显的频散;在高饱和度下纵波速度的频散变得明显.从干燥到完全水饱和条件,不同频率测量的致密砂岩的体积模量随岩石孔隙度增高而降低,且体积模量的变化量受岩石微观孔隙结构的影响较大.高孔、高渗砂岩无论在低含水度下还是在高含水饱和度下频散微弱,并且在地震频段下围压对于岩石纵横波速度的影响要大于频率的影响.高孔、高渗砂岩和致密砂岩不同含水饱和度下的频散差异可应用于储层预测,油气检测等方面,同时该研究可以更好地帮助理解岩石的黏弹性行为,促进岩石物理频散理论的发展,提高地震解释的精度.  相似文献   

10.
岩石从干燥状态下到饱和流体后纵波速度的变化情况对于地震速度预测、AVO分析以及流体识别具有重要意义,而有关泥质砂岩在干燥与饱和流体状态下纵波速度之间关系的研究甚少.因此本文利用三组实验数据研究了泥质砂岩在干燥与饱和流体状态下纵波速度之间关系的影响因素,并通过多元线性回归分析方法建立泥质砂岩饱和流体后的纵波速度与干燥状态下的纵波速度、孔隙度以及黏土含量之间的关系.研究表明:泥质砂岩在干燥与饱和流体状态下纵波速度之间的简单线性关系容易受到固结程度、孔隙流体性质以及围压的影响,而多元线性回归分析与简单线性分析相比,其拟合结果的判定系数明显提高,标准误差明显减小.此外,本文首次提出黏土含量与孔隙度比的概念(CPR),发现CPR与泥质砂岩饱和流体前后纵波速度差之间有很好的正相关性,随着CPR的增加,纵波速度差也表现出增大的趋势,CPR的提出为解释流体替换过程中岩石物理属性的变化情况提供了新的思路.  相似文献   

11.
We investigated initiation and propagation of compaction bands (CB) in six wet and four dry Bentheim sandstone samples deformed in axial compression tests with strain rates ranging from 3.2 × 10?8 s?1 to 3.2 × 10?4 s?1. Circumferential notches with 0.8-mm width and 5-mm depth served to initiate CB at mid-sample length. Wet samples were saturated with distilled water and deformed at 195 MPa confining pressure and 10 MPa pore pressure. Dry samples were deformed at 185 MPa confining pressure. Twelve P-wave sensors, eight S-wave sensors and two pairs of orthogonally oriented strain-gages were glued to the sample surface to monitor acoustic emission (AE), velocities and local strain during the loading process. Nucleation of compaction bands is indicated by AE clusters close to the notch tips. With progressive loading, AE activity increased and AE hypocenters indicated propagation of a single CB normal to the sample axis. CB propagation from the sample periphery towards the centre was monitored. Microstructural analysis of deformed samples shows excellent agreement between location of AE clusters and CBs. In both dry and wet samples the lateral propagation of CBs was about 100 times faster than axial shortening rates. At the slowest displacement rate, AE activity during band propagation was reduced and CB nucleation in wet samples occurred at 20% lower stresses. This may indicate an increasing contribution of stress corrosion processes to the formation of the compaction bands. In dry and wet samples inelastic compaction energy per area ranged between 16 and 80 kJ m?2. This is in good agreement with previous estimates from laboratory and field studies.  相似文献   

12.
单轴压缩下干燥和饱水岩石中超声P波的衰减   总被引:1,自引:0,他引:1       下载免费PDF全文
根据脉冲传播和频谱比方法的基本原理建立了一套超声波衰减和波速测量系统。研究了单轴压缩下超声P波在干燥和饱水的小浪底砂岩和房山大理岩中的衰减和速度。常压下,水饱和样品的Q_P值低于干燥样品。初始加载时,在大多数情况下,Q_p值明显增加即衰减减小;当应力水平达破裂强度50-60%后,岩石开始膨胀,Q_p减小即衰减增加;临近破裂Q_p减至最小。Q_p的变化量达一个数量级。单轴压缩下,在干燥和饱水的砂岩、大理岩中,V_p分别增加为27%和28%,44%和11%。径向Q_p和V_p随单轴压力的变化比轴向小得多,呈现明显各向异性。在本实验条件下,波在裂纹表面的摩擦耗散是主要的衰减机制,水的作用主要是潮湿和润滑裂纹表面,促进滑动,增加衰减。  相似文献   

13.
We investigated systematically the micromechanics of compaction in two carbonates of porosity above 30%, Majella grainstone and Saint Maximin limestone. The composition, grain size and pore surface area of these rocks were determined. Hydrostatic compression experiments were performed under dry and wet conditions beyond the onset of grain crushing. A significant water weakening effect was observed in both rocks. A set of conventional triaxial experiments was also performed on both rocks under dry conditions at confining pressures ranging from 3 to 31 MPa. Microstructural observations were carried out on the deformed samples. The mechanical behavior of these high porosity carbonates is dominated by shear-enhanced compaction associated in most cases with strain hardening. Stress-induced cracking and grain crushing are the dominant micromechanisms of deformation in both rocks. In Majella grainstone, compactive shear bands appeared at low confinement, in qualitative agreement with the deformation bands observed in the field. At higher confining pressures, compaction localization was inhibited and homogeneous cataclastic flow developed. In Saint Maximin limestone, compaction localization was observed at all confining pressures. An increasing number of compactive shear bands at various orientations appeared with increasing strain. These new data suggest that compaction localization is important in the mechanical compaction of high porosity carbonates.  相似文献   

14.
固原重塑黄土动力特性共振柱试验研究   总被引:1,自引:1,他引:0       下载免费PDF全文
利用GCTS共振柱测试仪研究了干密度和固结压力对固原黄土重塑土动剪切模量和阻尼比的影响及试验数据误差的基本规律。通过设计不同工况的试验条件,对比分析结果表明:相同含水率条件下,最大动剪切模量G_(dmax)随固结压力和干密度的增大而增大。相同干密度条件下,黄土的动剪切模量比随围压的增大而增大;阻尼比随围压的增大而减小;相同围压条件下,黄土动剪切模量比随干密度的增大而增大,阻尼比随干密度的增大而减小;不同剪应变特征点的动剪切模量比和阻尼比试验数据呈现一定的离散性,且离散程度阻尼比明显高于动剪切模量比。研究成果可为该地区场地地震反应分析及工程建设提供基础资料。  相似文献   

15.
土的最大动剪切模量、剪应变幅和阻尼比是对土层进行动力反应分析的重要力学参数。利用英国GDS公司生产的RCA共振柱仪,研究围压对都江堰地区粉质粘土的上述动力学参数的影响。研究表明:相同围压条件下,最大动剪切模量、剪应变幅和阻尼比随重复次数基本不变,表明该试验过程具有可重复性;最大动剪切模量、剪应变幅和阻尼比均受围压影响较大,随着围压的增大,最大动剪切模量和阻尼比均逐渐增大,而剪应变幅随着围压的增大逐渐减小。据此,建立了都江堰地区粉质粘土动力学参数随围压变化的经验公式。本研究可为土层地震动力反应分析提供参考并积累基础资料。  相似文献   

16.
Cracks play a very important role in many geotechnical issues and in a number of processes in the Earth’s crust. Elastic waves can be used as a remote sensing tool for determining crack density. The effect of varying crack density in crystalline rock on the P- and S-wave velocity and dynamic elastic properties under confining pressure has been quantified. The evolution of P- and S-wave velocity were monitored as a suite of dry Westerly granite samples were taken to 60, 70, 80 and 90 % of the unconfined uniaxial strength of the sample. The damaged samples were then subjected to hydrostatic confining pressure from 2 MPa to 200 MPa to quantify the effect of varying crack density on the P- and S-wave velocity and elastic properties under confining pressure. The opening and propagation of microcracks predominantly parallel to the loading direction during uniaxial loading caused a 0.5 and 6.3 % decrease in the P- and S-wave velocity, respectively. During hydrostatic loading, microcracks are closed at 130 MPa confining pressure. At lower pressures the amount of crack damage in the samples has a small but measureable effect. We observed a systematic 6 and 4 % reduction in P- and S-wave velocity, respectively, due to an increase in the fracture density at 2 MPa confining pressure. The overall reduction in the P- and S-wave velocity decreased to 2 and 1 %, respectively, at 50 MPa. The elastic wave velocities of samples that have a greater amount of microcrack damage are more sensitive to pressure. Effective medium modelling was used to invert elastic wave velocities and infer crack density evolution. Comparing the crack density results with experimental data on Westerly granite samples shows that the effective medium modelling used gave interpretable and reasonable results. Changes in crack density can be interpreted as closure or opening of cracks and crack growth.  相似文献   

17.
— The influence of differential stress on the permeability of a Lower Permian sandstone was investigated. Rock cylinders of 50 mm in diameter and 100 mm length of a fine-grained (mean grain size 0.2 mm), low-porosity (6–9%) sandstone were used to study the relation between differential stress, rock deformation, rock failure and hydraulic properties, with a focus on the changes of hydraulic properties in the pre-failure and failure region of triaxial rock deformation. The experiments were conducted at confining pressures up to 20 MPa, and axial force was controlled by lateral strain with a rate ranging from 10?6 to 10?7 sec?1. While deforming the samples, permeability was determined by steady-state technique with a pressure gradient of 1 MPa over the specimen length and a fluid pressure level between 40 and 90% of the confining pressure. The results show that permeability of low-porosity sandstones under increasing triaxial stress firstly decreases due to compaction and starts to increase after the onset of dilatancy. This kind of permeability evolution is similar to that of crystalline rocks. A significant dependence of permeability evolution on strain rate was found. Comparison of permeability to volumetric strain demonstrates that the permeability increase after the onset of dilatancy is not sufficient to regain the initial permeability up to failure of the specimen. The initial permeability, which was determined in advance of the experiments, usually was regained in the post-failure region. After the onset of dilatancy, the permeability increase displays a linear dependence on volumetric strain.  相似文献   

18.
Adopting the method of forced oscillation, attenuation was studied in Fontainebleau sandstone (porosity 10%, permeability 10 mD) at seismic frequencies (1–100 Hz). Confining pressures of 5, 10, and 15 MPa were chosen to simulate reservoir conditions. First, the strain effect on attenuation was investigated in the dry sample for 11 different strains across the range 1 × 10?6–8 × 10?6, at the confining pressure of 5 MPa. The comparison showed that a strain of at least 5 × 10?6 is necessary to obtain a good signal to noise ratio. These results also indicate that nonlinear effects are absent for strains up to 8 × 10?6. For all the confining pressures, attenuation in the dry rock was low, while partial (90%) and full (100%) saturation with water yielded a higher magnitude and frequency dependence of attenuation. The observed high and frequency dependent attenuation was interpreted as being caused by squirt flow.  相似文献   

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