相控误差法在少井区岩性分布研究中的应用

以塔里木盆地东北地区石炭系为例进行少井波阻抗反演,以此结果研究砂泥岩发育位置、剖面形态和厚度.波阻抗资料可分辨最小厚度为20 m,比常规剖面分辨率(30 m)高,可用于沉积相分析.但是用波阻抗资料进行泥岩视厚度计算,所得结果与钻井揭示厚度相比,相对误差为 12%~-15%.经过误差分析得知,相对误差与含泥率服从单峰态分布规律,且受沉积相控制.采用相控误差法校正泥岩视厚度得到真厚度,计算结果为勘探阶段烃源岩预测提供科学依据.     

陆相汕藏中砂泥岩互层时移地震遮掩效应及其对时移地震资料解释的影响

从差异波形特征的角度出发,分析时移地震差异波形特征与砂泥岩互层油藏中油层速度变化的关系.通过建立由5层地层组成的楔形地质模型,运用褶积公式及时移地震求差公式,得到泥岩速度为2 400 m/s和砂岩速度为2 700 m/s条件下,互层中砂岩速度变化±150 m/s的时移地震响应.研究结果表明砂泥岩互层的差异波形是一个多峰复合波,泥岩夹层的厚度是决定差异波形特征的一个主要因素,并且存在一个临界值,即四分之一主波长;如果泥岩夹层的厚度小于这一临界值,就会发生遮掩效应,即顶部油层的时移地震响应可以掩盖中、下部油层的时移地震响应.     

Carbonate Diagenesis Controlled by Glacioeustatic Sea-Level Changes： A Case Study from the Carboniferous-Permian Boundary Section at Xikou, China

The diagenesis of modern and ancient carbonatesedi ments has been widely studied and systematicallyreviewed since the 1960s (e .g. Moore ,2001 ,1989 ;Wang et al ., 1994 , 1991 ; McIlreath and Morrow,1990 ; Tucker and Bathurst , 1990 ; Schneidermannand Harris , 1985 ; Longman, 1980 ; Bathurst ,1975) . With the development of sequence stratigra-phy and its more widespread application, discussionabout the relationship between diagenesis and se-quence stratigraphy/sea-level changes ,as well as…     

金沙江某库区东爷庙滑坡成因分析及稳定性评价

文章在对滑坡周界确定和滑坡体特征研究基础之上,从岩性条件、地质构造及地下水等方面详细分析了滑坡成因。该滑坡发生在侏罗系沙溪庙组(J2s)缓倾角红层中,地层岩性为河湖相紫红色泥质粉砂岩、泥岩和灰绿色粉砂岩互层,软硬相间,该套地层的岩性内在差异构成了滑坡产生的岩性条件。加上边坡呈顺向坡结构,顺坡向节理发育,坡角临空,岩体沿着软弱层发生滑移-拉裂破坏。通过对滑坡进行稳定性计算和分析,结果表明:该滑坡在天然状态、蓄水或地震等不利条件下,整体仍处于稳定状态,只是在相对较陡的滑坡体前缘和库水位附近地形较陡的局部部位,蓄水后可能会产生小规模失稳,但其方量不会太大,加上离坝址较远,所以不会危及工程安全。因此,通过对滑坡成因分析和稳定性评价,为工程建设和移民安置工作提供了重要的保证。     

Effect of Overpressure on Rock Frame and Its Implications for Overpressure Evolution

Overpressure is a hot topic in the study of sedimentary basins. It is important in generation,maturation migration,and accumulation of hydrocarbon,but the effects of overpressure on rock frame have not been investigated. In this study,experiments were carried out to study the effects of overpressure on rock frame structures using five core samples from the Junggar basin,Northwest China. The deformations and velocities for the samples were measured at different effective pressures related to non-equilibrium compaction and fluid expansion overpressure mechanisms. The results show that the effect of overpressure on rock frames gradually increases when the effective pressure drops down to a certain value (called critical pressure). Moreover,non-equilibrium compaction mechanism has more effects on rock frames than fluid expansion mechanism under the same effective pressure. Furthermore to study rock frame structural changes,we use Kuster and Toks?z's expressions to simulate the effective aspect ratios of inclusions α (penny shapes) for different effective pressures. The results show that the α decreases dramatically when the effective pressure decreases from the critical pressure. Changes of α can be interpreted as responses to the rock frame changes when grains conform one another by rotating and self-adjusting. However,different mechanisms of overpressure have different effects on rock frames. The rock frame can be affected more easily by overpressure in shallow regions generated by non-equilibrium compaction mechanism. Once this kind of rock frames are preserved after overpressure releases to a normal hydrostatic pressure,they can be identified by their specific rock frame characters. This method provides a new way to study overpressure release and fluid migration and accumulation.     

超压盆地中泥岩的流体压裂与幕式排烃作用

流体压裂是在异常高流体压力体系的低渗泥岩中流体活动的主要输导通道。流体压裂不仅导致低渗泥岩的幕式压实作用,而且为油气运移,储集的研究提供了新的理论模式。超压盆地泥岩的压实演化可划分为两个阶段,即连续压实和幕式压实阶段,其中幕式压实阶段又可根据导致流体压裂的主控因素进一步划分为两个亚阶段,即水力压裂和生烃压裂,前者主要由于泥岩欠压实和新生流体源的增压所致,后者则主要由于泥岩中有机质生烃及烃类裂解后增     

根据含超压气体裂隙震源模式讨论P波初动符号的分布

利用含超压气体裂隙震源模式［１］分析研究了Ｐ波初动符号的分布．根据理论推导,不同倾角含超压气体裂隙可分别形成Ｐ波初动符号的四象限分布图象和圆、椭圆、抛物线、双曲线等圆锥曲线形Ｐ波节线．按节线形状和失稳方式进行了地震分类．所推论的初动Ｐ波、Ｓ波振幅分布规律和地形变特征都与实际相符     

淮北煤田上石盒子组花斑泥岩中的粘土矿物研究

淮北煤田上石盒子组花斑泥岩中的粘土矿物组合以高岭石为主,伊利石次之。高岭石的结晶度较好。伊利石均表现有混层现象。研究表明,花斑泥岩经历了较强的成岩作用。     

歧深地区双超压系统发育特征及油气成藏效应

在钻井实测储层压力(DST)、计算泥岩压力及地震资料解释的基础上,对歧深地区超压体系发育特征、分布规律和成藏效应进行了深入分析,认为歧深地区具有"三层压力结构,两个超压系统"特征。压力结构在纵向上可以划分为常压系统、上部弱超压系统和下部超压系统。超压从东营组开始出现,歧口凹陷中心超压最强,北大港东翼、歧口凹陷及板桥凹陷超压次之。双超压结构对歧深地区油气聚集有明显的控制作用,从而形成了"上油下气"分布格局,由此建立了"双压控藏"模式。