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利用纵波AVAZ方法反演小尺度垂直裂缝密度
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摘要
裂缝性储层已经成为当今油气勘探的重点,与此同时,利用地球物理探测方法描述储层裂缝性质也越来越受到人们的关注。实际上,地层上覆载荷的压实等作用使得高角度和近于垂直的裂缝易被保存下来。垂直裂缝发育带的存在会引起地震波传播特征的方位各向异性,即波在传播时由于方向或偏振的变化而引起物理性质测量值的变化。另外,纵波勘探是目前最经济和实用的勘探技术,因此可以通过提取纵波速度、振幅和衰减等地震波特征的方位各向异性来研究垂直裂缝发育带。然而,目前对裂缝发育带的描述多为定性描述,对裂缝发育带裂缝密度的定量描述方法很少。在前人工作基础之上,本文重点研究利用相交测线上纵波反射振幅差信息反演裂缝密度。主要研究对象是HTI介质和含有两组不同尺度的垂直裂缝介质。
     首先,本文基于各向异性介质的本构关系,利用求解横向各向同性介质的Christoffel方程得到相速度与群速度表达式,进而分析地震波传播规律。介绍并比较了三种等效HTI介质理论即Hudson理论、线性滑动理论和Thomsen裂缝理论。因为裂缝性质的变化会对弹性参数的影响进而对Thomsen参数产生影响,所以三个Thomsen参数值以及它们之间的关系可以揭示HTI介质裂缝密度与裂缝类型。另外,根据各向异性程度不同的HTI介质的纵波反射系数随入射角和方位角变化特征分析,可选取出对反射振幅最敏感的Thomsen参数。
     其次,虽然在理论上AVAZ特征可以很好的揭示裂缝走向,但是在实际应用中仍面临观测系统和工区地质情况等方面的限制。本文针对Emilio地区,合理选取面元并利用该面元上纵波AVAZ响应估计裂缝走向。利用AVAZ响应分析裂缝走向结果与Emilio地区测井数据得到的裂缝走向基本相符,验证了本文利用纵波AVAZ响应估计裂缝走向的方法在Emilio地区中应用的可行性。
     再次,本文分析了HTI介质的三分量地震记录中的反射特征。提出了对多组相交测线上纵波AVAZ响应差运用遗传算法反演HTI介质裂缝密度方法。另外,该方法在反演前运用利用SVD对多组相交测线上纵波AVAZ响应差去噪。通过直接对AVAZ响应与AVAZ响应差运用SVD去噪结果的对比,验证了基于AVAZ响应差研究裂缝性质的优越性。基于数值模拟的AVAZ响应运用该方法反演得到的裂缝密度值接近模型值,验证了算法的可行性。
     最后,本文假设介质背景是均匀各向同性且包含两组不同尺度的垂直裂缝。分析当大尺度垂直裂缝裂隙屈服度变化或小尺度裂缝包含物状态变化时,大尺度裂缝的存在对利用新算法反演小尺度裂缝密度结果的影响。利用本文提出的反演方法得到的结果与模型裂缝密度值误差分析揭示了新的算法在多尺度裂缝模型中的适用范围。
Nowadays, fractured reservoir has already been a big picture of oil and gasexploration, at the same time, description of fractured reservoir by using geophysicalexploration method is getting more and more attention. In fact, the overlying stratapressure may cause high-angle fracture and vertical fracture can be easily kept. Theexisting development zone of vertical fracture may cause azimuthal anisotropy ofseismic wave propagation characteristics which means measured value of physicalfeatures varies with the direction or polarization of wave propagation. What’s more Pwave exploration is the most economical and practical exploration technology atpresent, so we can research on the development zone of vertical fracture by gettingazimuthal anisotropy of seismic characterizations, such as P wave velocity, amplitudeand attenuation. However, descriptions of fracture development zone is qualitative sofar and there is only a few methods for quantitative description of fracture density. Onthe basis of predecessors’ work, the research in this paper focus on inversion offracture density by using the difference information of P wave reflection amplitudebetween two crossing line. The main study objects are HTI media and the media withtwo vertical scale fractures.
     Firstly,based on constitutive relationship of anisotropic media, we can getexpressions of phase velocity and group velocity by solving Christoffel equation fortransversely isotropic media and study on seismic wave propagation law. Thenintroduce and compare three theories of equivalent transversely isotropic media with ahorizontal symmetry axis including Hudson theory, linear slip deformation theory andThomsen fracture theory. The changes of fracture characteristics will play influenceon elastic parameters, then Thomsen parameters will be also influenced. What’s more, according to the analysis on P wave reflection coefficient variation with incident angleand azimuth for HTI media with different anisotropy, we can choose the mosesensitive Thomsen parameter to reflection amplitude.
     Secondly, AVAZ response can reveal fracture strike very well in theory, but westill need face the limitation of observing system,geological conditions and so on.Aiming at Emilio area, we reasonably choose a bin and use P wave AVAZ responsegetting from it to estimate fracture strike in this paper. The fracture strike got by usingAVAZ response and from well log result are coincide and that verifies the feasibilityof estimating fracture strike by using P wave AVAZ response in Emilio area.
     Thirdly, we analysis reflection characteristics form three component seismicrecord for HTI media in this paper. Then come up with a fracture density inversionmethod based on multiple group difference of AVAZ response from crossing lines.What’s more, we use SVD on the multiple group difference of AVAZ response fromcrossing lines to reduce noise before inversion using this method. Through comparethe results of reducing noise between directly using SVD on AVAZ response andusing SVD on AVAZ response difference, we testify the advantage of studying onfracture characteristics based on AVAZ response difference. The inversion value offracture density based on AVAZ response from numerical simulation approaches themodel value which testify the feasibility of this algorithm.
     At last, assume that background of the media is isotropic homogeneous and themedia contain two sets of vertical fractures with different scales. Then analysis theinfluence of small-scale fracture density which is inversion result estimated by usingthe new algorithm cased by large-scale fracture when fracture compliance of verticallarge-scale fracture or what filled in small-scale fracture is changing. The erroranalysis of inversion result got by applying the new algorithm and the value offracture density reveals the range of application for multi-scale fracture model by using the new algorithm.
引文
[1]沈金松,苏本玉,郭乃川.裂缝性储层的电各向异性响应特征研究[J].地球物理学报,2009,52(11):2903-2912.
    [2]曲鸿雁,周生田.裂缝性油藏开发技术进展[J].内蒙古石油化工,2009,(8):106-107.
    [3]张国君,冯晅,王典等.裂隙性油气藏发展现状[J].吉林大学学报(地球科学版),2008,38(增刊):43-47.
    [4]邓友茂.三维地震裂缝介质正反演研究[D].成都理工大学,2008.
    [5]赵诚亮,李瑞,邓雁等.裂缝性储层地震识别技术[J].天然气技术与经济,2011,5(1):17-20.
    [6]周亚楠,邓媛,霍威等.油气储层裂缝描述综述[J].辽宁化工,2012,41(10):1008-1011.
    [7]朱兆林,王永刚,曹丹平.裂缝性储层AVO检测方法综述[J].勘探地球物理进展,2004,27(2):87-92.
    [8]刘书强,胡前泽.叠前裂缝检测技术浅谈[J].吐哈油气,2008,13(1):68-70.
    [9]石双虎.基于新等效介质模型HTI介质中断裂大小、各向异性及频率之间的依赖关系[D].吉林大学,2007.
    [10]童亨茂.储层裂缝描述与预测研究进展[J].新疆石油学院学报,2004,16(2):9-13.
    [11]Stuart C, Peacock S. A review of the current understanding of seismic shear-wavesplitting in the Earth's crust and common fallacies in interpretation[J].WaveMotion,2008,45(6):675-722.
    [12]Thomsen L. Weak elastic anisotropy[J].Geophysics,1986,51(10):1954-1966.
    [13]Berryman J G. Long-wave elastic anisotropy in transversely isotropic media[J].Geophysics,1979,44(5):896-971.
    [14]Byun B S. Seismic parameters for transversely isotropic media[J].Geophysics,1984,49(11):1908-1914.
    [15]李振春,李娜,黄建平等.裂缝介质横波分裂时差影响因素定量研究[J].地球物理学进展,2013,28(1):240-249.
    [16]Lynn H B, Bates C R, Simon K M. Azimuthal anisotropy in P-wave3-D(multiazimuth) data[J].The Leading Edge,1996,15(9):923-928.
    [17]Sena A G. Seismic traveltime equations for azimuthally anisotropic and isotropicmedia: Estimation of interval elastic properties[J].Geophysics,1991,56(2):2090-2101.
    [18]Tsvankin I. Reflection moveout and parameter estimation for horizontaltransverse isotropy[J].Geophysics,1997,62(2):614-629.
    [19]Stuart C, Robert M, Bamford D. Estimating crack parameters from observationsof P-wave velocity anisotropy[J].Geophysics,1980,45(3):345-360.
    [20]Li X. Fracture detection using azimuthal variation of P-wave moveout fromorthogonal seismic survey lines[J].Geophysics,1999,64(4):1193-1201.
    [21]周辉,何樵登.横向各向同性介质走时反演[J].石油物探,1995,34(3):63-68.
    [22]张雨晴,王志章.致密碎屑岩裂缝性储层预测方法综述[J].科技导报,2010,28(14):109-112.
    [23]张建伟,陈天胜,宁俊瑞等.利用纵波AVA进行裂缝储层和流体识别[J].物探化探计算技术,2009,31(6):594-597.
    [24]桂志先,段天友,易远元等.裂缝性储层纵波地震检测方法研究[J].石油天然气学报(江汉石油学院学报),2007,29(4):75-79.
    [25]杨晓,王真理,喻岳任.裂缝型储层地震检测方法综述[J].地球物理学进展,2010,25(5):1785-1794.
    [26]Feng S, Jesus S, Daniel R B, et al. Azimuthal offset-dependent attributes appliedto fracture detection in a carbonate reservoir[J].Geophysics,67(2):355-364.
    [27]殷八斤,曾灏,杨在岩. AVO技术的理论与实践[M].北京:石油工业出版社,1995.
    [28]Koefoed O.Reflection and transmission coefficients for plane longitudinalincident waves[J].Geophysics,1961,10(3):304-351.
    [29]Aki. K. I., G. R. P. Quantitative seismology: theory and methods[M].SanFrancisco: W H Freeman and Co,1980.
    [30]Shuey R. T. A simplification of the Zoeppritz equations[J].Geophysics,1985,50(4):609-614.
    [31]Rutherford S. R., Williams R. H. Amplitude-versus-offset variations in gassands[J]. Geophysics,1989,54(6):680-688.
    [32]Castagna J. P., W. S. H. Principles of AVO crossplotting[J].The Leading Edge,Society of Exploration Geophysicists,1997,17:337-342.
    [33]John P. C., Herbert W. S., Foster D. J. Framework for AVO gradient and interceptinterpretation[J].Geophysics,1998,63(3):948-956.
    [34]Keith C. M., Crampin S. Seismic body waves in anisotropic media: reflection andrefraction at a plane interface[J].Geophys J Roy Astr Soc,1977,49(1):181-208.
    [35]Daley P F, Hron F. Reflection and transmission coefficients for transverselyisotropic media[J].Bulletin of the Seismological Society of America,1977,67(3):661-675.
    [36]Daley P F, Hron F. Reflection and transimission coefficients for seismic waves inellipsoidally anisotropic media[J].Geophysics,1979,44(1):27-38.
    [37]Daley P. F., Hron F. SH waves in layered transversely isotropic media-anasymptotic expansion approach[J].Bulletin of the Seismological Society ofAmerica,1979,69(3):689-711.
    [38]Thomsen L. Weak anisotropic reflections, in Offset dependent reflectivity[M].Eds: Soc. Expl. Geophys,1993.
    [39]Banik N. C. An effective anisotropy parameter in transversely isotropic media[J].Geophysics,1987,52(12):1654-1664.
    [40]Schoenberg M., J. P.'Zoeppritz' rationalized and generalized to anisotropy[J].Journal of Seismic Exploration,1992,1(1):125-144.
    [41]Rüger A. P-wave reflection coefficients for transversely isotropic models withvertical and horizontal axis of symmetry[J].Geophysics,1997,62(3):713-722.
    [42]Václav V, Ivan P. PP-wave reflection coefficients in weakly anisotropic elasticmedia[J].Geophysics,1998,63(6):2129-2141.
    [43]David G., Kim H. V.. Fracture detection in Manderson Field:A3-D AVAZ casehistory[J].The Leading Edge,2000,19(11):1214-1221.
    [44]Lynn H B, Simon K M, Bates C, et al. Azimuth anisotropy in P-wave3-D(multiazimuth) data[J].The Leading Edge,1996,15(8):923-928.
    [45]Stephen A. Hall, Kendall J.-M. Fracture characterization at Valhall:Application ofP-wave amplitude variation with offset and azimuth (AVOA) analysis to a3Docean-bottom data set[J].Geophysics,2003,68(4):1150-1160.
    [46]Hall S A, J-Michael K, Barkved O. Fractured reservoir characterization usingP-wave AVOA analysis of3D OBC data[J].The Leading Edge,2002,21(8):777-781.
    [47]He Chen, John P. Castagna, Raymon L. Brown, et al. Three-parameter AVOcrossplotting in anisotropic media[J].Geophysics,2001,66(5):1359-1363.
    [48]何樵登,陶春辉.用遗传算法反演裂隙各向异性介质[J].石油物探,1995,34(3):46-50.
    [49]Varela I. Fracture Studies from Amplitude versus Offset and Azimuth and VerticalSeismic Profile data[D].University of Edinburgh,2009.
    [50] Morten J, Enru L, Chapman M. Estimation of anisotropic permeability infractured reservoirs from seismic AVOZ analysis[M].SEG. San Antonio.2007.
    [51]Peimin Zhu, Jiaying Wang, Wenhui Yu, et al. Inverting reservoir crack densityfrom P-wave AVOA data[J].Journal of Geophysics and Engineering,2004,1(2):147-152.
    [52]朱培民,王家映,於文辉等.用纵波AVO数据反演储层裂隙密度参数[J].石油物探,2001,40(2):1-12.
    [53]刘财,刘宇巍,冯晅等.基于方位相交的纵波AVA数据运用SVD反演HTI介质裂缝密度[J].吉林大学学报(地球科学版),2013,43(5):1655-1662.
    [54]Chapman M, Wu X. Bayesian inversion of AVOZ data for fracture, rock and fluidproperties[M].EAGE. London.2013.
    [55]何樵登,张中杰.横向各向同性介质中地震波及其数值模拟[M].吉林大学出版社,1996.
    [56]Hudson J. A. Overall properties of a cracked solid[J].Proc Camb Phil Soc,1980,88(2):371-384.
    [57]Hudson J. A. Wave speeds and attenuation of elastic waves in material containingcracks[J].Geophys J Roy Astr Soc,1981,64(1):133-155.
    [58]Stuart C. Effective elastic constants for wave propagation through crackedsolids[J].Geophys J Roy Astr Soc,1984,76(1):135-145.
    [59]Schoenberg M. Elastic wave behavor across linear slip interfaces[J].Journal of theAcoustical Society of America,1980,68(5):1516-1521.
    [60]杨德义,王赟,张美根.弱度比在裂隙含流体检测中的应用[J].地球物理学报,2011,54(3):862-866.
    [61]Hsu C. J., Schoenberg M. Elastic waves through a simulated fracturedmedium[J].Geophysics,1993,58(7):964-977.
    [62]Schoenberg M, Sayers C. Seismic anisotropy of fractured rock[J].Geophysics,1995,60(1):204-211.
    [63]Schoenberg M, Douma J. Elastic wave propagation in media with parallelfractures and aliged cracks[J].Geophysical Prospecting,1988,36(6):571-590.
    [64]Thomsen L. Elastic anisotropy due to aligned cracks in porousrock[J].Geophysical Prospecting,1995,43(6):805-829.
    [65]Tsvankin I. Reflection moveout and parameter estimation for horizaontaltransverse isotropy[J].Geophysics,1997,62(2):614-629.
    [66]Bakulin A, Grechka V, Tsvankin I. Estimation of fracture parameters fromreflection seismic data—Part I: HTI model due to a single fractureset[J].Geophysics,2000,65(6):1788-1802.
    [67]刘财,刘洋,王典等.均匀倾斜层状地层中地震波球面扩散补偿方法研究[J].地球物理学进展,2004,19(3):590-595.
    [68]Zheng Y. Seismic azimuthal anisotropy and fracture analysis from PP reflectiondata [D].Calgary,Alberta,2006.
    [69]Gaiser J, Loinger E, Lynn H, et al. Birefringence analysis at Emilio field forfracture characterization[J].First Break,2002,20(8):505-514.
    [70]Laura V, Eugenio L, James G, et al.3D/4C Emilio:Azimuth processing andanisotropy analysis in a fractured carbonate reservoir[J].The Leading Edge,2003,22(7):675-679.
    [71]刘海波,全海燕,陈浩林等.海上多波多分量地震采集综述[J].中国石油勘探,2007,3):52.57.
    [72]王玉贵,李庆春,朱光明.浅海区多波地震勘探资料采集处理系统试验[J].西安工程学院学报,2002,24(2):51-54.
    [73]王银年.遗传算法的研究与应用[D].江南大学,2009.
    [74]姚姚.地球物理反演基本理论与应用方法[M].中国地质大学出版社,2002.
    [75]明亮.遗传算法的模式理论及收敛理论[D].西安电子科技大学,2006.
    [76]徐树方.矩阵计算的理论[M].北京:北京大学出版社,1995.
    [77]李平,王椿墉,许厚泽等.地球物理反演中奇异值分解应用的若干问题探讨[J].自然科学进展,2001,11(8):891-896.
    [78]郝雪,李月,杨宝俊.基于奇异值分解和小波闽值方法的地震资料处理方法[J].吉林大学学报(地球科学版),2006,36(专辑):44-48.
    [79]Isabel V, Sonja M, Li X. Fracture density inversion from a physical geologicalmodel using azimuthal AVO with optimal basis functions[C]. SEG. Houston.2009.
    [80]Isabel V, Maultzsch S. Azimuthal AVO Inversion for Fracture Characterization: Anew techique using Singular Value Decomposition[C]. EAGE. London.2007.
    [81]吴如山,安艺敬一,李欲澈.地震波的散射和衰减[M].北京:地震出版社,1993.
    [82]尹军杰,刘学伟,李文慧.地震波散射理论及应用研究综述[J].地球物理学进展,2005,20(1):123-134.

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