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1.
中国大陆科学钻探(CCSD)680-1200米区段发育了多个韧性剪切带,带中主要岩石类型包括片麻岩和超高压榴辉岩。片麻岩中的变形石英、面理化榴辉岩中的拉长石榴石和绿辉石的应变轴比都表现为X>Y>Z,Flinn系数分别为0.11-0.27、0.22-0.23和0.23-0.24。随着糜棱岩化作用的增强,变形石英的C轴组构由Z轴极密逐渐向Y轴极密和叶理面上的大圆环带转变。在常温常压下测试了样品的波速,计算出片麻岩Vp和Vs的各向异性分别为30.17%-60.97%和11.52%-35.79%,榴辉岩Vp和Vs的各向异性分别为0.17%-11.19%和2.41%-6.70%。影响各向异性的主要因素有岩石的结构构造、矿物的晶格优选方位(LPO)、形态优选方位(SPO)和定向微裂隙。随着糜棱岩化作用的增强,岩石的P波各向异性逐 渐升高。变形岩石中的黑云母、石英、绿辉石的LPO和SPO是地震波各向异性的主要控制因素。饱水后的片麻岩样品的P波各向异性明显低于干燥片麻岩样品。在东海钻井中的强反射带主要是由于不同岩层之间的波阻抗差异而造成的,榴辉岩/强退变榴辉岩和黑云斜长片麻岩之间的接触界面会产生较强的地震深反射。此外,与LPO相关的地震波各向异性会增强地震波的反射,所以韧性剪切带中的糜棱岩化片麻岩可能是地震反射的良好载体。韧性剪切带中岩石弹性波速度的强各向  相似文献   

2.
为了研究水化岩石圈地幔和地幔楔的地震波速、各向异性及其与蛇纹石化程度及应变状态的关系,作者实验测量了8块叶蛇纹岩(采自辽宁的岫玉)标本在不同构造主方向(X,Y和Z)上的纵、横波速度随围压(0~600 MPa)的变化规律,详细研究了叶蛇纹石在塑性变形过程中通过(001)[010]位错滑移形成很强的晶格优选定向和高达21%的纵波速度各向异性与24%的剪切波分裂的特征,发现高温叶蛇纹岩与低温利蛇纹岩具有截然不同的地震波性质,例如,在围压600 MPa下,高温叶蛇纹岩的Vp=6.73 km/s、Vs=3.74 km/s,Vp/Vs=1.80,而低温利蛇纹岩的Vp=5.10 km/s、Vs=2.32 km/s,Vp/Vs=2.20。前人利用低温蛇纹石化橄榄岩的波速数据解释温度高于300℃的水化地幔楔和岩石圈地幔的地震波速不可避免地要低估研究区域内蛇纹石化的程度和水含量。本研究查明叶蛇纹岩的地震波性质及其各向异性特征亦为解释全球大洋板块俯冲带乃至青藏高原地区的剪切波分裂资料提供了新的思路。  相似文献   

3.
大别山榴辉岩的密度和波速及其对壳—幔循环的启示   总被引:7,自引:0,他引:7  
测定了大别山地区榴辉岩和麻粒岩的密度和高温高压 (至 5 .0GPa和 130 0℃ )的纵波速度 (Vp)。超高压榴辉岩具有较高的密度和Vp 及较弱的各向异性。榴辉岩的压力系数为 0 .2 2~ 0 .33km/s·GPa ,超高压榴辉岩的温度系数为 - 3.41× 10 -4 km/s·℃。榴辉岩的密度和波速的分析表明 ,地幔深部的超高压榴辉岩形成后可能包含了两个过程 ,即一部分榴辉岩通过拆沉作用进入深部地幔 ,另一部分快速折返至地壳内或地表 ,榴辉岩的形成过程代表了壳幔物质循环。现今的大别山深部可能只存在少量榴辉岩。  相似文献   

4.
在1.0GPa、常温至1100℃条件下测量了角闪石斜长片麻岩的纵波速度(Vp),并统计了不同温度实验产物中各种矿物的体积百分含量。结果显示,1.0GPa下,角闪石斜长片麻岩的Vp首先随温度升高(室温至700℃)缓慢降低约6%,然后(700—850℃)快速降低约6%,再(850~950℃)转而急剧升高15%~25%,最后(T〉950℃)又快速下降。实验产物分析表明在高温高压下α-石英-β石英相变和岩石部分熔融是岩石Vp异常变化的主要因素。由取样产物的矿物含量和弹性参数,计算了各温度条件下岩石的Vp得出与实验测量相同的波速-温度变化趋势,即Vp随温度升高先缓慢降低,接着快速降低后又急剧升高,最后又快速减小。实验测量和理论计算对比研究表明,通过高温高压下岩石中的物相变化观测结果进行岩石波速的计算,是检验岩石弹性波速测量结果和研究地球内部地震波结构的一种有效方法。  相似文献   

5.
徐海军  金振民  欧新功 《岩石学报》2006,22(7):2081-2088
在常温常压条件下获得了中国大陆科学钻探(CCSD)主孔331块岩心的磁化率各向异性(AMS)数据,并建立了主孔100—2000m的体积磁化率和AMS连续剖面。数据统计分析显示,主孔100—2000m岩心的磁化率(κ)介于1.05×10-4SI和0.12SI之间,几何平均值为1.855×10-3SI;磁化率各向异性度(Pj)介于1.04和2.10之间,几何平均值为1.155。该井段出露的主要岩石类型有榴辉岩、退变质榴辉岩、角闪岩、正片麻岩、副片麻岩和蛇纹石化橄榄岩,它们的垂向分布特征控制着磁化率剖面的变化。主孔的超高压变质岩石在折返过程中普遍经历了强烈的角闪岩相退变质作用的改造。其磁化率特征也发生相应的改变。蛇纹石化橄榄岩具有很高的磁化率(8.58×10-2SI)和各向异性度(1.335)。这主要源于橄榄岩蛇纹石化过程中产生的大量磁铁矿。榴辉岩、退变质榴辉岩和角闪岩代表榴辉岩从新鲜到完全退变质的三个阶段,它们的磁化率和磁化率各向异性度分别为榴辉岩(1.28×10-3SI、1.077)、退变质榴辉岩(3.19×10-3SI、1.206)、角闪岩(1.02×10-3SI、1.104)。正片麻岩的磁化率和各向异性度分别为5.34×10-3SI和1.167。副片麻岩的磁化率和各向异性度分别为3.46×10-4SI和1.150。对58个变形岩石的AMS测试结果显示,其磁化率椭球体的主轴方向与岩石组构基本一致,即最大磁化率主轴κ1平行矿物线理,最小磁化率主轴κ3垂直岩石面理。同时,这些变形岩石的AMS椭球体多呈现明显的压扁状特征,反映超高压变质岩石在折返过程中处于强烈挤压变形的构造应力环境,为苏鲁超高压变质板片的挤出折返模式提供了佐证。该研究成果也为超高压变质岩石地区磁学研究、地球物理调查和测井成果的解释提供了重要的实验约束。  相似文献   

6.
系统研究了中国大陆科学钻探工程主孔100~2000米岩石的热导率和生热率特征。初步研究了岩石热导率随矿物组成的变化关系、岩石热导率的各向异性及其影响因素。主孔2000米的岩心热导率介于1.873~4.062Wm^-1K^-1之间,平均热导率2.967Wm^-1K^-1。整体上热导率出现的频率主峰分布在2.8~3.0Wm^-1K^-1。榴辉岩热导率随着其退变质程度的增加而降低,新鲜榴辉岩热导率集中分布于3.6~3.7Wm^-1K^-1,角闪石化榴辉岩的热导率分布在3.1~3.2Wm^-1K^-1,强退变的榴辉岩热导率分布于2.4~2.5Wm^-1K^-1。片麻岩热导率主要分布于2.8~3.0Wm^-1K^-1。从垂向上看,主孔100~735米主要由榴辉岩组成,热导率整体比较大,平均3.265Wm^-1K^-1;1200~1600米主要以花岗质片麻岩为主,热导率比其它层位偏低,平均2.755Wm^-1K^-1。通过对面理发育的样品进行测试,东海地区各类岩石的热导率具有较明显的各向异性。榴辉岩和片麻岩热导率的各向异性平均值分别为4、66%和22.99%,超基性岩的热导率平均值为3.322Wm^-1K^-1,各向异性16.08%。岩石热导率在垂直于面理的方向上具有最小值,在平行于面理的方向上具有最大值。上述资料对超高压地体热结构特征的研究提供了重要数据基础。  相似文献   

7.
随着页岩气勘探开发工作的不断深入,地震相关勘探技术在页岩气钻井部署和页岩气富集带或"甜点"区评价中发挥重要作用。不同应力环境下岩石的弹性波速及其各向异性实验数据是地震资料叠前反演的重要约束性基础资料,对深部页岩气地球物理探测、储层评价及甜点预测具有重要意义。本文以湘西桑页1井龙马溪组页岩、五峰组页岩及底板泥灰岩钻孔岩芯为研究对象,实验测量了不同应力条件下岩芯的弹性波速特征,计算了应力环境下的波速差异,并对比了页岩与泥灰岩的波速各向异性。结果表明,在5~100 MPa应力环境下,粉砂质、硅质和含粉砂页岩的纵波速度分别为4.8~5.1 km/s、5.1~5.3 km/s和5.2~5.5 km/s,泥灰岩的纵波速度在5.9~6.4 km/s之间;原位应力环境下,页岩与泥灰岩的纵波速度差异介于14.9%~21.7%之间;受微裂缝和层理面的影响,页岩垂直层理方向纵波速度明显低于平行层理方向,而泥灰岩的纵波速度为平行层理方向明显高于垂直层理方向。  相似文献   

8.
利用超高压变质岩的P波速度估算地下岩石的热导率   总被引:3,自引:0,他引:3  
岩石热导率是了解地球内部热传导过程的重要参数之一, 但热导率的测量在室内和野外都比较复杂.如何利用容易获得的岩石物理参数(如超声波速度) 来估算岩石的热导率就显得非常重要.通过对中国大陆科学钻探(CCSD) 主孔655件样品热导率和超声波速度的相关分析, 把样品分为新鲜榴辉岩、退变质榴辉岩、副片麻岩和正片麻岩4类, 并分别建立了利用岩石P波速度估算热导率的计算方程.回归计算表明, 榴辉岩热导率和P波速度之间的相关性较大, 相关系数在0.7左右, 片麻岩显示的相关系数比较小, 在0.4~0.5之间.鉴于样本数量较大, 这种结果足以表明热导率和P波速度之间可以用给定的线性关系来表达.为了检验获得的方程, 在CCSD主孔中选取典型的岩性单元, 利用测得的P波速度估算相应的热导率, 结果显示估算值和实测热导率平均值非常接近, 表明利用P波估算岩石热导率的方程是可行和实用的, 为本区和相似地区大地热流和热结构计算提供了热导率的计算方法和依据, 因而具有重要的岩石物理学和地球物理意义.   相似文献   

9.
中国大陆科学钻探主孔自然放射性测井及其解释   总被引:3,自引:0,他引:3  
为了认识江苏东海超高压变质带上地壳岩石自然放射性的垂向分布特征, 榴辉岩退变质程度对放射性元素浓度的影响, 以及放射性产热率对地温梯度的影响, 利用中国大陆科学钻探(CCSD) 主孔100~5000m自然放射性测井(自然伽马和自然伽马能谱) 资料统计了CCSD主孔各类岩石的自然放射性强度和铀、钍、钾元素的浓度, 计算出产热率曲线.自然伽马, 铀、钍、钾浓度和产热率从蛇纹岩到榴辉岩、角闪岩、副片麻岩、正片麻岩依次增大.随着榴辉岩退变质程度的增强, 其铀、钍、钾元素的浓度值逐渐增大.CCSD主孔自然放射性的垂向分布特征主要受岩性控制, 自然放射性随深度增加有增强趋势.产热率与自然伽马测井值之间有很好的线性关系, 在高放射性岩层的上部, 地温梯度会出现较强扰动和低值异常.   相似文献   

10.
CCSD主孔100~2950m榴辉岩、退变榴辉岩类岩石叶理倾角明显较片麻岩类岩石叶理倾角陡,前者总体倾角55°左右,后者28°左右,局部可见片麻岩类叶理切割榴辉岩类叶理,因此两者叶理可能形成于不同时期;两类岩石之间现部分为韧性剪切带接触关系,韧性剪切带形成于苏鲁地体折返主期自SEE向NWW的韧性剪切作用。榴辉岩、退变榴辉岩类岩石叶理产状对发育于该类岩石内的微断层产状有一定控制作用,而片麻岩类岩石叶理产状对发育于该类岩石内的微断层产状控制作用相对较弱。孔区脆性变形主要反映白垩纪以来SEE-NWW向伸展构造应力场的变形特征,主孔100~1620m倾伏向以SEE向占绝对优势的微正滑断层擦痕即为该期变形的产物。  相似文献   

11.
About 30 samples representing major lithologies of Sulu ultrahigh-pressure (UHP) metamorphic rocks were collected from surface exposures and exploration wells, and compressional (Vp) and shear wave (Vs) velocities and their directional dependence (anisotropy) were determined over a range of constant confining pressures up to 600 MPa and temperatures ranging from 20 to 600 °C. Samples range in composition from acidic to ultramafic. P- and S-wave velocities measured at 600 MPa vary from 5.08 to 8.64 km/s and 2.34 to 4.93 km/s, respectively. Densities are in the range from 2.60 to 3.68 g/cm3. To make a direct tie between seismic measurements (refraction and reflection) and subsurface lithologies, the experimental velocity data (corresponding to shallow depths) were used to calculate velocity profiles for the different lithologies and profiles of reflection coefficients at possible lithologic interfaces across the projected 5000-m Chinese Continental Scientific Drilling Program (CCSD) crustal segment. Comparison of calculated in situ velocities with respective intrinsic velocities suggests that the in situ velocities at shallow depths are lowered by an increased abundance of open microcracks. The strongly reflective zone beneath the Donghai drill site can be explained by the impedance contrasts between the different lithologies. Contacts between eclogite/peridotite and felsic rocks (gt-gneiss, granitic gneiss), in particular, may give rise to strong seismic reflections. In addition, shear-induced (lattice preferred orientation (LPO)-related) seismic anisotropy can increase reflectivity. For the explanation of the high velocity bodies (>6.4 km/s) around 1000 m and below 3200-m depth, large proportions of eclogite/peridotite (about 40 and 30 vol.%, respectively) are needed.  相似文献   

12.
M.G. Kopylova  J. Lo  N.I. Christensen 《Lithos》2004,77(1-4):493-510
Modes and compositions of minerals in Slave mantle xenoliths, together with their pressures and temperatures of equilibrium were used to derive model depth profiles of P- and S-wave velocities (Vp, Vs) for composites equivalent to peridotite, pyroxenite and eclogite. The rocks were modeled as isotropic aggregates with uniform distribution of crystal orientations, based on single-crystal elastic moduli and volume fractions of constituent minerals. Calculated seismic wave velocities are adjusted for in situ pressure and temperature conditions using (1) experimental P- and T- derivatives for bulk rocks' Vp and Vs, and (2) calculated P- and T- derivatives for bulk rocks' elastic moduli and densities. The peridotite seismic profiles match well with the globally averaged IASP91 model and with seismic tomography results for the Slave mantle. In peridotite, an observed increase of seismic wave velocities with depth is controlled by lower degrees of chemical depletion in the deeper upper mantle. In eclogite, seismic velocities increase more rapidly with depth than in peridotite. This follows from contrasting first-order pressure derivatives of bulk isotropic moduli for eclogite and peridotite, and from the lower compressibility of eclogite at high pressures. Our calculations suggest that depletion in cratonic mantle has a distinct seismic signature compared to non-cratonic mantle. Depleted mantle on cratons should have slower Vp, faster Vs and should show lower Poisson's ratios due to an orthopyroxene enrichment. For the modelled Slave craton xenoliths, the predicted effect on seismic wave velocities would be up to 0.05 km/s.  相似文献   

13.
The Peloritani Mountain Belt (north-eastern Sicily) represents the connection between the Southern Appenninic Range and the Appenninic Maghrebid Chain. The lithotypes outcropping in a 36 km long and approximately 8 km wide area in the eastern part of the Peloritani Mountains are considered to represent most properly the composition of the lower crust. We selected 7 representative samples of silicate rocks (amphibolite, paragneisses, augen gneiss, phyllitic quartzite, pegmatitic rock) and 3 samples of calcite rocks (calc-schist, marbles) for the petrophysical measurements. Measurements were done on sample cubes of dry rocks in a multi-anvil apparatus. Raising of pressure gives rise to velocity increase, but the rate is different in the silicate and calcite rocks and closely related to progressive closure of microcracks. Linear behaviour is approached above about 200 MPa. Increasing temperature at 600 MPa decreases velocities in most silicate and in the calcite rocks with almost linear slopes. Substantial anisotropy of P- and S-wave velocities and shear wave splitting is found in both rock types. The residual anisotropy observed above about 200 MPa is attributed to lattice preferred orientations (LPO) of major minerals. 3D velocity calculations for an amphibolite, a paragneiss and a marble sample based on the LPO of hornblende, biotite and calcite, respectively, confirm the experimental findings of a close relationship between velocity anisotropy, shear wave splitting, shear wave polarization, lattice preferred orientation and the structural frame of the rocks (foliation, lineation). In the silicate rocks, the intrinsic (600 MPa) average P-wave velocities and Poisson's (Vp / Vs) ratios exhibit a tendency for a linear increase with densities, whereas the three calcite rocks cluster at markedly higher P-wave velocities and Poisson's (Vp / Vs) ratios, compared to their densities. In the silicate rocks, there is also a linear trend for an inverse relationship between the SiO2 content, density and the Poisson's (Vp / Vs) ratio, respectively.  相似文献   

14.
中国大陆科学钻探孔区三维地震资料的初步解释   总被引:19,自引:8,他引:19  
利用中国大陆科学钻探岩心、测井与VSP资料来标定地震反射体,大大提高了大陆科学钻探孔区地质构造解释的可信度。超高压变质带地壳波速特征主要表现在上地壳顶部的高速层,其厚度一般小于10km;其下方正常的中下地壳波速结构反映了中新生代地壳的拉张与伸展。孔区三维地震拱形反射由榴辉岩及切穿它们的晚期破碎带共同形成的。在CCSD主孔东南方深部重力高部位有多个这样的拱形反射,预示在地表陡倾榴辉岩的延伸方向还有多个一定规模的隐伏榴辉岩体。孔区广泛发育韧性剪切带,韧性剪切带产生强反射的主要机制是韧性剪切复合岩套,由糜棱岩和经剪切错动产生的表壳岩片互层组成。三维地震调查提供了三维的反射地震波场,使揭示孔区三维的地质构造成为可能。450ms以上的时间切片与地袁地质构造和地磁异常相关,而1000~1200ms的时间切片与深部重力异常相关,主要反映由隐伏榴辉岩体产生的反射波场.根据上述研究结果,编制了沿三维地震主剖面的推断地质构造图。  相似文献   

15.
The 3-D P- and S-wave velocity models of the upper crust beneath Southwest Iberia are determined by inverting arrival time data from local earthquakes using a seismic tomo~raphy method. We used a total of 3085 P- and 2780 S-wave high quality arrival times from 886 local earthquakes recorded by a per- manent seismic network, which is operated by the Institute of Meteorology (IM), Lisbon, Portugal. The computed P- and S-wave velocities are used to determine the 3-D distributions of Vp/Vs ratio. The 3-D velocity and Vp/Vs ratio images display clear lateral heterogeneities in the study area. Significant veloc- ity variations up to ~6% are revealed in the upper crust beneath Southwest lberia, At 4 km depth, both P- and S-wave velocity take average to high values relative to the initial velocity model, while at 12 km, low P-wave velocities are clearly visible along the coast and in the southern parts. High S-wave velocities at 12 km depth are imaged in the central parts, and average values along the coast; although some scattered patches of low and high S-wave velocities are also revealed. The Vp/Vs rztio is generally high at depths of 4 and 12 km along the coastal parts with some regions of high Vp/Vs ratio in the north at 4 km depth, and low Vp/Vs ratio in the central southern parts at a depth of 12 km, The imaged low velocity and high Vp/Vs ratios are related to the thick saturated and unconsolidated sediments covering the region; whereas the high velocity regions are generally associated with the Mesozoic basement rocks.  相似文献   

16.
The ratio of P- to S-wave velocities (Vp/Vs) is regarded as one of the most diagnostic properties of natural rocks. It has been used as a discriminant of composition for the continental crust and provides valuable constraints on its formation and evolution processes. Furthermore, the spatial and temporal changes in Vp/Vs before and after earthquakes are probably the most promising avenue to understanding the source mechanics and possibly predicting earthquakes. Here we calibrate the variations in Vp/Vs in dry, anisotropic crustal rocks and provide a set of basic information for the interpretation of future seismic data from the Wenchuan earthquake Fault zone Scientific Drilling (WFSD) project and other surveys. Vp/Vs is a constant (φ0) for an isotropic rock. However, most of crustal rocks are anisotropic due to lattice-preferred orientations of anisotropic minerals (e.g., mica, amphibole, plagioclase and pyroxene) and cracks as well as thin compositional layering. The Vp/Vs ratio of an anisotropic rock measured along a selected pair of propagation-vibration directions is an apparent value (φij) that is significantly different from the value for its isotropic counterpart (φ0). The usefulness of apparent Vp/Vs ratios as a diagnostic of crustal composition depends largely on rock seismic anisotropy. A 5% of P- and S-wave velocity anisotropy is sufficient to make it impossible to determine the crustal composition using the conventional criteria (Vp/Vs<1.756 for felsic rocks, 1.756l.944 fluid-tidied porous/fractured or partially molten rocks) if the information about the wave propagation-polarization directions with respect to the tectonic framework is unknown. However, the variations in Vp/Vs measured from borehole seismic experiments can be readily interpreted according to the orientations of the ray path and the polarization of the shear waves with respect to the present-day principal stress directions (I.e., the orientation of cracks) and the frozen fabric (I.e., foliation and lineation).  相似文献   

17.
中国大陆科学探井岩性的VSP地震特征分析   总被引:1,自引:0,他引:1  
中国大陆科学钻探(CCSD)井位于苏鲁超高压变质带南部,地处郯庐断裂东侧的东海县境内。VSP地震勘探为CCSD多学科研究内容之一,利用数字地震仪(HF300)和多级三分量数字检波器(GeoChain)对探井进行了VSP测量。结合VSP勘探结果和CCSD探井5000 m岩性资料,分析了井中岩性分段特征、超高压变质岩的地震响应特征和vp/vs比值特征,取得了若干具有科学意义的结论:(1)以榴辉岩的分布和组合特征进行的岩性分段比较合理,每段的VSP速度和测井密度等特征和岩性分布具有很好的一致性。(2)榴辉岩与片麻岩界面以及剪切带均可形成强反射,正/副片麻岩界面也可产生明显反射,透镜状和条带状岩体的反射同相轴呈现不同程度的弯曲,剪切带的反射同相轴连续性好。(3)榴辉岩以高波速(6.3 km/s)、低vp/vs值(1.2)和波组强而稀疏为特征,副片麻岩以较高波速(6.1 km/s)、高vp/vs值(1.8)和波组较稀疏为特征,正片麻岩以较低波速(5.8 km/s)、中等vp/vs值(1.5)和波组较密集为特征,而剪切带以强反射、vp/vs值最高(2.2)为特征,而且不论剪切带出现在哪种岩性中其vp/vs值都很高。该研究成果不但揭示了变质带的地震响应特征,同时为二维或三维地面地震解释提供科学依据,减少解释分析中的多解性和不确定性,能够有效地提高中国大陆科学钻探孔区地质构造解释的可信度,为其他学科研究提供依据。  相似文献   

18.
大陆科学钻探为认识深部地壳的结构、组成、力学性质和物理状态提供了重要的基础数据。岩石物理性质的测量对于原位测井资料的校正和地表地球物理测量的解释具有重要意义,岩石物理性质和岩石学研究相结合,还能为岩石的变质作用以及变质过程中化学成分的迁移提供必要的约束。本文主要对CCSD100-3100m的综合岩石物理资料进行了相关性调查和聚类分析,并得出如下结论:(1)岩石物理性质中的地震波速度、密度、热导率之间具有强相关性,他们都受岩石中主要矿物的组成和含量所控制;(2)岩石的电阻率和磁化率受金属氧化物含量的控制,与岩性有相关性;孔隙度、渗透率与岩性没有相关性;(3)利用岩石的物理性质可以反演不同的岩性,其中地震波速度、密度和热导率对榴辉岩和片麻岩大类具有很好的分类效果,而结合磁化率和电阻率则能更好的区分出超基性岩、正片麻岩和副片麻岩。上述结论对综合地球物理解释中物理参数的选取和结晶岩区地球物理解释标尺的建立具有重要的意义。  相似文献   

19.
We have measured P- and S-wave velocities on two amphibolite and two gneiss samples from the Kola superdeep borehole as a function of pressure (up to 600 MPa) and temperature (up to 600 °C). The velocity measurements include compressional (Vp) and shear wave velocities (Vs1, Vs2) propagating in three orthogonal directions which were in general not parallel to inherent rock symmetry axes or planes. The measurements are accompanied by 3D-velocities calculations based on lattice preferred orientation (LPO) obtained by TOF (Time Of Flight) neutron diffraction analysis which allows the investigation of bulk volumes up to several cubic centimetres due to the high penetration depth of neutrons. The LPO-based numerical velocity calculations give important information on the different contribution of the various rock-forming minerals to bulk elastic anisotropy and on the relations of seismic anisotropy, shear wave splitting, and shear wave polarization to the structural reference frame (foliation and lineation). Comparison with measured velocities obtained for the three propagation directions that were not in accordance with the structural frame of the rocks (foliation and lineation) demonstrate that for shear waves propagating through anisotropic rocks the vibration directions are as important as the propagation directions. The study demonstrates that proper measurement of shear wave splitting by means of two orthogonal polarized sending and receiving shear wave transducers is only possible when their propagation and polarization directions are parallel and normal to foliation and lineation, respectively.  相似文献   

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