沁水盆地柿庄北深部煤层水平井CO2注入参数研究

基于CO₂的吸附能力大于CH₄的原理,向深部煤层中注入并封存CO₂同时置换驱替CH₄增加煤层气井产量,具有环境和经济双重效益。研究深部煤储层特征,通过气、水两相多组分,单孔和双孔模型的三维储层数值模拟技术,模拟不同井底压力下,完成注入量所需要的时间。优化后的注入施工参数为井口注入压力低于10MPa,注入速率低于47 L/min。根据数值模拟结果选定注入压力,注入结果与模拟连续注入时间一致,说明该方法可以有效地模拟注入压力和注入量之间的关系,保障CO₂注入施工安全有效。     

超临界CO2岩石致裂机制分析

超临界CO2是一种介于气体和液体之间的特殊状态的CO2流体,具有低黏、高扩散性和零表面张力等独特的性质。利用超临界CO2作为压裂液,有助于裂缝的起裂和扩展,同时可避免储层伤害。通过研究超临界CO2射流破岩和压裂特性,分析得到了超临界CO2岩石致裂机制。研究结果表明,超临界CO2低黏等特性使其更容易进入岩石微孔和微缝之中,在岩石内部建立大小不一的流体压力系统,使岩石发生拉伸和剪切破坏;常规流体压裂起裂压力较高,裂缝一般为单条或多条平直裂缝,大多沿着同一方向贯穿强度较高的胶结颗粒,且裂缝断面光滑、平整;超临界CO2压裂起裂压力相比于常规流体压裂低,在岩石中形成的裂缝网络较为复杂,裂缝互相连通,一般沿着强度较低的胶结物开裂,较少贯穿胶结颗粒,裂缝断面较为粗糙。该研究结果可为超临界CO2压裂技术的实施提供理论支撑。     

二维随机介质模型正演指导复杂地层地震解释——以薄层砂泥岩交互地层为例

大港油田砂泥岩交互地层存在着非均质复杂地质形态,为保证其精细解释效果,根据随机过程理论,提出了选用二维指数型椭圆自相关函数为复杂非均质地质体进行简化建模的方法。正演算法使用交错网格有限差分法模拟弹性波在二维随机介质模型中的传播,激发方式使用自激自收模式。正演结果表明,随机介质模型模拟大港油田薄层砂岩互层地层具有合理性,交错网格有限差分算法对于该模型的正演数值模拟,算法合适。     

CaCl2溶液对不同黏土基防渗墙渗透性的影响

在垃圾填埋场和场地污染防治工程中,黏土基防渗墙作为原位屏障,已广泛应用于隔离污染物与控制污染地下水的迁移。由黏土与地层混合形成的防渗墙与CaCl2溶液相互作用后,其渗透性会发生怎样的变化。针对这一问题,使用福建标准砂模拟砂性地层,以4种黏土作为混合材料,通过混合、浇筑和固结以后,对其渗透系数和水分特征曲线进行了实测。结果表明,在10%黏土添加量下,当4种砂-黏土混合土经0.2 mol/L CaCl2溶液渗透稳定后,其渗透系数相比渗透液为自来水时都有不同程度的增大,但渗透系数增大的倍数没有超过10。此外,CaCl2溶液在4种砂-黏土混合土中渗透稳定后试样的孔隙率没有发生较大变化,只是小幅地减小了。试验结果分析认为,钙离子与黏土矿物颗粒表面的单价阳离子发生了置换反应,使扩散双电层厚度减小,结合水含量降低,因而有效孔隙率增加,可能是宏观上造成渗透系数变大的主要原因。     

高效液相色谱-紫外光谱分析氢醌-双(β-羟乙基)醚

建立了高效液相色谱-紫外光谱法测定聚氨酯扩链剂氢醌-双(β-羟乙基)醚(HQEE)工业品中HQEE主含量和对苯二酚残留的方法。在氰基柱上,以甲醇-水-1%乙酸溶液(体积比10∶50∶40)为流动相,流速1.0 mL/min时,HQEE、对苯二酚及其他相关杂质得到良好分离,紫外光谱285 nm检测。方法简便、快捷,结果准确可靠,在工业生产中可有效地指导HQEE合成过程的质量控制。     

陕北新庄地区延长组长2油层组储层特征

一般河道砂体的正粒序性决定了其下部物性条件优于上部,但新庄地区长2油层组河道砂体的物性特征截然相反,而是中上部物性条件好,下部物性条件普遍差.在储层岩石学特征、孔隙类型等研究的基础上,对此进行了探讨,认为造成其特殊性的原因主要是由于压实、胶结、次生加大等作用.指出河道边滩砂体中上部储层为该区的主力储层.     

Seal integrity and feasibility of CO<Subscript>2</Subscript> sequestration in the Teapot Dome EOR pilot: geomechanical site characterization

This paper reports a preliminary investigation of CO₂ sequestration and seal integrity at Teapot Dome oil field, Wyoming, USA, with the objective of predicting the potential risk of CO₂ leakage along reservoir-bounding faults. CO₂ injection into reservoirs creates anomalously high pore pressure at the top of the reservoir that could potentially hydraulically fracture the caprock or trigger slip on reservoir-bounding faults. The Tensleep Formation, a Pennsylvanian age eolian sandstone is evaluated as the target horizon for a pilot CO₂ EOR-carbon storage experiment, in a three-way closure trap against a bounding fault, termed the S1 fault. A preliminary geomechanical model of the Tensleep Formation has been developed to evaluate the potential for CO₂ injection inducing slip on the S1 fault and thus threatening seal integrity. Uncertainties in the stress tensor and fault geometry have been incorporated into the analysis using Monte Carlo simulation. The authors find that even the most pessimistic risk scenario would require ∼10 MPa of excess pressure to cause the S1 fault to reactivate and provide a potential leakage pathway. This would correspond to a CO₂ column height of ∼1,500 m, whereas the structural closure of the Tensleep Formation in the pilot injection area does not exceed 100 m. It is therefore apparent that CO₂ injection is not likely to compromise the S1 fault stability. Better constraint of the least principal stress is needed to establish a more reliable estimate of the maximum reservoir pressure required to hydrofracture the caprock.     

The Glueckstadt Graben of the North-German Basin: new insights into the structure from 3D and 2D gravity analyses

The structure of the Glueckstadt Graben has been investigated by use of 3D gravity backstripping technique and by 2D gravity and magnetic modelling. Subtracting the gravity effects of the Meso-Cenozoic sediments together with Permian salt reveals a positive residual anomaly within the Glueckstadt Graben. This anomaly includes two local maxima over the Westholstein and Eastholstein Troughs. The 2D gravity models point to the presence of a high-density body within the lower crust of the Glueckstadt Graben. In addition, the results of 2D magnetic modelling indicate that the central part of the high-density body is overlain by an area with high susceptibility. Most probable, the formation of this high-density body is a result of complex poly-phase tectonic history of the study area. Finally, the results of gravity modelling indicate that Permian salt is not homogeneous. 3D gravity analysis and, especially, 2D gravity modelling have distinguished the differences in degree of salt saturation in salt-rich bodies, and elucidate the proportion of Rotliegend salt.