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Geomechanical Simulation of 3D Directional Borehole Circumference in Deep Composite Salt Formation 深层复合盐层中三维定向钻孔周长的地质力学模拟
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-04-30 DOI: 10.2113/2024/lithosphere_2023_212
Shiyuan Li, Chenglong Li, Zhaowei Chen, Wenbao Zhai, Yajun Lei, Jiawei Cao
Composite salt formation is a high-quality caprock for oil and gas resources. The accident encountered in composite salt formation drilling is a big problem to be solved in the drilling process. According to statistics, nearly 50% of drilling accidents occur in composite salt formations. The composite salt formation is mainly composed of salt, gypsum, and interbed mud, and the lithology is complex and changeable. Therefore, it is very important to study the deformation mechanism and leading influencing factors of composite salt formation in view of the problem of frequent accidents in the drilling process. In this article, the creep parameters based on the constitutive equation of creep of salt rock are obtained by combining theoretical with experimental research. A three-dimensional directional wellbore mechanical model is established to analyze the influence of inclination on borehole shrinkage.The salt gypsum layer refers to the formation with salt or gypsum as the main component. In the oil drilling industry, we usually regard the formation as mainly composed of sodium chloride or other water-soluble inorganic salts such as potassium chloride, magnesium chloride, calcium chloride, gypsum, or Glauber’s nitrate as the salt gypsum formation, that is, the salt gypsum layer. According to statistics, salt rocks in sedimentary basins are the best caprock, under which are buried a considerable amount of oil and gas resources in the world, especially rich unconventional oil and gas resources [1-3]. Therefore, the salt gypsum layer is not only the focus of the world oil industry but also the focus of our oil and gas resource development.Along with the process of oil and gas exploitation, the shallow, easily recoverable resources are gradually exhausted, and the exploitation center is gradually transferred to the deep oil and gas resources. The salt rock with very low permeability and porosity is the best caprock, and the drilling of salt rock is unavoidable in the drilling process. The gypsum rocks, which are mainly composed of salt or gypsum, exist above oil and gas reservoirs. The gypsum rocks found in our drilling are mainly distributed in Tarim, Jianghan, Sichuan, Shengli, Zhongyuan, North China, Xinjiang, Qinghai Changqing, and so forth. Various accidents occurred in the drilling of the gypsum rocks in the above oil fields, such as sticking and squeezing casing.Hambley et al. [4] improved the creep constitutive model of salt rock by fully combining the experimental and field data. Fossum et al. [5] determined the stress-related probability distribution function through the pure salt creep test and creep model. Weidinger et al. [6] established a composite plastic deformation model to explicitly consider the heterogeneity of the observed dislocation structure and calculated the transient creep and steady-state creep of salt rock with this model combined with the mechanical laws of dislocation motion. Urai et al. [7] discussed the process of dissolut
[13]提出合理使用盐水泥浆,通过调整氯(Cl-)和氯化钠(NaCl)的浓度来平衡井筒中盐岩的溶解速率和收缩速率,从而防止堵塞和卡钻。Zeng 等[14]以岩石力学为基础,分析了钻井液密度对钻井后深层盐膏岩层蠕变的影响,提出了盐膏岩层蠕变压力的计算模型。Zhang等[15]分析了塔河油田盐膏地层钻井的难点,采用RWD(边钻边扩)、合理的钻井组装、适宜的钻井液密度钻井盐膏地层。曾[16]对深井石膏盐层取样进行蠕变实验,分析蠕变压力的变化,绘制钻井液密度图,并结合石膏盐岩的溶解规律,提出了合理钻井液的确定方法,并在实际钻井中得到应用。Zhao 等[17]通过实验认为,层状盐岩是一种特殊的软岩组合,弹性模量较小,侧向变形能力较大。Ye 等人[18]通过现场分析认为,在复合盐岩层的钻进过程中,聚砜欠饱和盐硅酸盐钻井液能很好地满足钻进过程中的地质要求,适当调整 Cl- 含量可实现盐岩收缩与盐岩溶解的动态平衡。Zeng 等[19]建立了盐岩、砂、泥岩互层复合盐层在三向原位应力作用下井眼收缩的有限元三维模型,得到了盐层在泥浆密度作用下的井眼收缩值。Xu 等[20]通过单轴压缩、三轴压缩和蠕变实验获得了盐岩的力学特征参数,并分析了层状盐岩的蠕变机理。Ma 等人[21] 对人工压制的盐岩样品进行了蠕变试验,确定其蠕变规律与天然岩芯的蠕变规律相似。他们还通过三轴蠕变实验确定了不同矿物成分含量对蠕变的影响,得出了高含量样品稳态蠕变速率较低的结论。Chen等[22]在理论模型分析的基础上,确定了石膏岩蠕变的主要影响因素和蠕变直径收缩的直接因素,并提出了一种通过扭转钻孔直径收缩来预测卡滞时间的方法。Zhao等[23]通过微观分析了复合盐地层的矿物成分和理化功能,分析了井壁失稳的机理,并综合各种因素选择了适合复合盐地层的钻井液密度和成分。Lin等[24]建立了盐岩-软泥岩-盐岩三维复合盐层模型,并绘制了钻井液密度图,考虑了软泥岩与盐石膏层之间的蠕变。针对盐层定向钻井的研究,Zeng 等[19]建立了盐岩、砂岩、泥岩互层复合盐层在三向原位应力作用下井眼收缩的有限元三维模型,得到了盐层随泥浆密度变化的井眼收缩率。Zhao等[23]通过微观分析了复合盐地层的矿物成分和物理化学功能,分析了井壁失稳的机理,并综合各种因素选择了适合复合盐地层的钻井液密度和成分。Lin等[24]建立了盐岩-软泥岩-盐岩三维复合盐层模型,并绘制了钻井液密度图,考虑了软泥岩与盐石膏层之间的蠕变。如果钻井过程中钻井液性能选择不当,就会在很短时间内出现井眼收缩、卡管、井壁坍塌等现象。盐层承载力低,钻井液柱压力超过岩石断裂压力容易产生拉裂,造成严重漏失。值得注意的是,关于井眼稳定性、直径减小、卡管和深层复合盐地层坍塌的研究已经很多。
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引用次数: 0
Mеsozoic Tectonothermal Evolution of the Zagan Metamorphic Core Complex in Western Transbaikalia: 40Ar/39Ar and FTA Dating 外贝加尔西部扎根变质岩核心复合体的新生代构造热演化:40Ar/39Ar和FTA年代测定
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-04-30 DOI: 10.2113/2024/lithosphere_2023_306
Mikhail M. Buslov, Anna V. Kulikova, Evgenii V. Sklyarov, Alexei V. Travin
A model of tectonothermal evolution of the Zagan metamorphic core complex (MCC) based on the new data from 40Ar/39Ar dating of amphibole, mica, and apatite fission-track dating is discussed. A relationship with the long-range impact of processes from the collision of the North China (Amurian–North China) block with the Siberian continent in the Mesozoic era is proposed. The Zagan MСС was formed in the Cretaceous period on the southern flank of a high mountain uplift of Western Transbaikalia, composed of late Paleozoic granitoids of the Angara–Vitim batholith. According to 40Ar/39Ar dating of amphiboles and micas from the mylonite zone, the active development time of the Zagan MCC corresponds to the early Cretaceous epoch (131, 114 Ma). The tectonic exposure of the core from about 15 km to the depths of about 10 km occurred at a rate of tectonic erosion of 0.4–0.3 mm/year as a result of post-collisional extension of the Mongol–Okhotsk orogen. Apatite fission-track dating shows that further exhumation and cooling of the rocks to about 3 km occurred in the lower-upper Cretaceous epoch (112, 87 Ma). The erosional denudation rate was about 0.3 mm/year.MCC- metamorphic core complexes, AFT- apatite fission-trackMesozoic metamorphic core complexes (MCCs) [1-3] are common in East Asia. They mark global intracontinental extensions along the folded borders of the Siberian craton in Western Transbaikalia and the North China craton [4-13]. The Zagan MCC is one of the more than ten identified ones on the southern border of the Siberian Craton [6-13], where Paleozoic magmatic complexes of the world’s largest Baikal–Vitim and Khentei batholithes and well-known Cenozoic Baikal rift zone occur. Currently, the tectonothermal history of the rocks of the region using apatite fission track dating has been published in a small number of papers [14, 15], partly in [16-19]. In the papers [14, 15], the analysis of geological and geophysical data and the results of track dating revealed the evolution of the relief and tectonic stages of the region formation along the NE-SW profiles from the Baikal-Patom Upland to the Barguzin Ridge, located, respectively, in the northwest and northeast of Lake Baikal. It was assumed, that the Baikal-Patom Upland was reactivated in the middle Jurassic–early Cretaceous epoch after the Mongol-Okhotsk orogeny, occurred in the vast convergence zone of the North Chinese (Amurian–North China block) and Siberian cratons. Apatite fission track dating of the Barguzin Ridge (block) indicates [15] that it intensively rose (rapid cooling phase) in the period of 65–50 Ma (Pliocene-early Eocene epoch) and in the last five Ma (Pliocene-Quaternary period).Tectonothermal evolution of the late Paleozoic granitoids of the Angara–Vitim batholith has been reconstructed using complex thermochronology, including U/Pb, 40Ar/39Ar, and partly fission track dating methods [16-18]. Closure temperatures of the isotope systems of zircon and amphibole show that the rapid
根据闪石、云母和磷灰石裂变轨道测年的 40Ar/39Ar 测年新数据,讨论了扎根变质岩核复合体(MCC)的构造热演化模型。提出了与中生代华北(阿穆尔-华北)地块与西伯利亚大陆碰撞过程的长程影响之间的关系。扎根СС形成于白垩纪,位于外贝加尔西部高山隆起的南侧,由安加拉-维季姆浴成岩的晚古生代花岗岩组成。根据对岩浆岩带的闪石和云母进行的 40Ar/39Ar 测定,扎根 MCC 的活跃发展时期与白垩纪早期(131-114Ma)一致。由于蒙古-鄂霍次克造山带碰撞后的延伸,岩芯从约15千米到约10千米深处的构造暴露以每年0.4-0.3毫米的构造侵蚀速度发生。磷灰石裂变轨迹测年显示,在白垩纪下-上世期(112, 87 Ma),岩石进一步剥蚀和冷却至约3 km。MCC-变质岩核复合体,AFT-磷灰石裂变径迹Mesozoic metamorphic core complexes(MCCs)[1-3] 在东亚很常见。它们标志着沿外贝加尔西部西伯利亚克拉通和华北克拉通褶皱边界的全球大陆内延伸[4-13]。扎根 MCC 是西伯利亚克拉通南部边界上已确定的十多个 MCC 之一[6-13],世界上最大的贝加尔湖-维季姆和肯特岩的古生代岩浆复合体以及著名的新生代贝加尔湖断裂带都位于这里。目前,利用磷灰石裂变轨道测年法研究该地区岩石构造热历史的论文为数不多[14, 15],部分发表在[16-19]中。在论文[14,15]中,对地质和地球物理数据的分析以及轨道测年的结果揭示了该地区形成的地貌和构造阶段的演变,沿东北-西南剖面,从贝加尔-帕托姆高地到巴尔古津海脊,分别位于贝加尔湖的西北和东北部。据推测,贝加尔湖-帕托姆高原是在蒙古-奥霍次克造山运动之后的中侏罗世-早白垩世重新激活的,发生在华北(阿穆尔-华北地块)和西伯利亚板块的巨大汇聚区。对巴尔古津海脊(区块)的磷灰石裂变轨迹测年表明[15],在 65-50 Ma(上新世-始新世早期)和最近 5 Ma(上新世-第四纪)期间,巴尔古津海脊强烈上升(快速冷却阶段)。利用复杂的热时学,包括 U/Pb, 40Ar/39Ar 和部分裂变轨道测年方法,重建了安加拉-维提姆岩床晚古生代花岗岩的构造热演化[16-18]。锆石和闪石同位素系统的闭合温度表明,安加拉-维季姆浴成岩在结晶后立即发生了急剧冷却,这表明在西伯利亚南部地区与广泛的晚古生代造山运动有关的时期,岩石发生了强烈剥蚀,厚度达 4-7 千米。二叠纪-侏罗纪早期(295,170Ma),以生物同位素系统逐渐关闭为特征的构造稳定纪之后,长石同位素系统在侏罗纪中期-白垩纪早期(170,140Ma)关闭。这一时期恰好是蒙古-奥霍次克造山带开始形成的时期,其特征是厚度约为 3 千米的剥蚀。在古新世-中新世时期(60, 5 Ma),西外贝加尔地区发生了缓慢的剥蚀。因此,根据现有的地质和地质年代数据,我们可以认为,在安加拉-维季姆熔岩花岗岩地区的西外贝加尔地区,曾发生过高达 6-8 千米的隆起。本文根据闪石、云母和磷灰石裂变轨迹测年的 40Ar/39Ar 新数据,讨论了扎甘 MCC 的构造-热演化模型,认为它是在高山隆起的边缘部分形成的构造。中生代MCC常见于外贝加尔西部西伯利亚克拉通靠近蒙古-奥霍次克缝合带的南部褶皱边界(图1)以及华北克拉通边界的褶皱带[4-13](图2)。
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引用次数: 0
Development of a Large Shaking Table Test for Sand Liquefaction Analysis 开发用于砂液化分析的大型振动台试验
IF 2.4 4区 地球科学 Q3 GEOCHEMISTRY & GEOPHYSICS Pub Date : 2024-04-30 DOI: 10.2113/2024/lithosphere_2024_137
Chuanqin Yao, Huaqiao Zhong, Zhehao Zhu
This article highlights the development of a large shaking table test for sand liquefaction analysis. Two soil containers of different sizes were fabricated. The first one was small (0.87 m × 0.87 m × 1.20 m) in which the reconstitution and saturation methods could be easily tested. The dry tamping (DT) method was used to fabricate a model specimen. The subsequent field measurements suggested that the DT method provided a good distribution of sand grains in different cross sections. Before supplying the model specimen with water, carbon dioxide was flushed to replace air bubbles. This helped in obtaining a good degree of saturation, later verified by a digital moisture meter. For a given inlet water flux, the recorded pore water pressure displayed a quasi-linear trend, suggesting a good internal void system. This reconfirms the effectiveness of the DT method to yield homogeneous model specimens. The second soil container was huge (4 m × 4 m × 2 m) and used to explore liquefaction behavior in real engineering dimensions. Flexible foams were mounted on the side walls to mitigate the boundary effect. Although the boundary effect still manifested itself near the edges of the container during base shaking, half of the model specimen underwent a correct simple shear condition. For further analysis, vane shear tests were carried out before and after the liquefaction test. It was found that the intermediate layer, in general, suffered from the most severe liquefaction failure.Research activities into sand liquefaction have been conducted since the 1964 Niigata earthquake in Japan [1, 2]. In the laboratory, monotonic and cyclic triaxial tests are widely adopted to investigate liquefaction responses. As for laboratory element tests, the state parameter (considering both relative density and consolidation stress [3, 4]) and degree of saturation are two decisive indicators [5, 6] for examining the liquefaction potential. Besides, the soil fabric [7, 8] formed in different specimen reconstitution methods [9-11] has recently been proven to be another influential factor in controlling liquefaction triggering.Although triaxial tests certainly provide valuable insights into the mechanism of sand liquefaction, the understanding based on these tests is still limited by the size effect and thus only represents the liquefaction behavior of a unit soil element. This is far from representing a natural soil extent subjected to seismic loading in a semi-infinite space. Therefore, shaking table tests play an increasingly important role in the context of geotechnical earthquake engineering and contribute to improving the understanding of the liquefaction phenomenon. Many successful configurations have been presented in the literature [12-17]. Teparaksa and Koseki [18] performed a series of liquefaction tests on a shaking table to assess the effect of liquefaction history on liquefaction resistance of level ground. Ko and Chen [19] investigated the evolution of mechanical p
该方法包括在侧壁上粘贴柔性泡沫,以抑制入射波的反射。最后进行了一次完整的液化实验,以检验上述缓解策略的有效性,并检测砂土液化的敏感区域。首先给出了所用沙子的指数特性。第三部分介绍了利用小型土壤容器开发的重组和饱和方法,随后对其性能进行了详细讨论。下一节将介绍在大型土壤容器中进行的巨型振动台液化试验的实验结果。最后,我们讨论了在基础摇动过程中观察到的边界效应以及相关的现场结果。在本研究中,液化分析采用了法国贫级配参考砂 Hostun 31(HN31)。该砂的平均粒度为 D50 = 0.35 mm,均匀系数为 Cu = D60/D10 = 1.57,最小空隙率为 emin = 0.656,最大空隙率为 emax = 1.00,特殊重力为 Gs = 2.65 [20,21]。除了空隙率和固结应力[3, 22, 23]之外,沉积方法[9, 24]被认为是影响砂液化演变的另一个决定性因素。从一般意义上讲,在振动台上制作均匀的砂试样时,普遍采用气冲法这种简便的方法。然而,在大规模实验中,砂粒在重力作用下的自由下落不可避免地会在试验大厅中产生厚厚的砂尘,这对 MTS 称重传感器是有害的。此外,在本研究中,几乎不可能实现能够容纳如此大量颗粒组件的砂斗。作为替代方案,我们选择了干捣实(DT)方法,并首先使用小型容器进行检验,以检查重组试样的均匀性。Zhu 等人[25] 在不排水三轴试验中使用 DT 方法制作了元件试样,从而证实了这种方法的可重复性。为了全面了解内部均匀性,人们将叶片剪切试验作为识别 DT 方法制作的试样质量的标准[26]。在岩土工程中,叶片剪切试验是一种方便的现场方法,用于估算给定深度土壤单元的剪切强度[27]。该试验用于现场测量既快速又经济。试验采用了市售的叶片剪切设备(由英安扬公司生产),主要包括:(i) 多根可达到最大深度 3 米的延长杆;(ii) 精度大于 10%的扭矩计。因此,如图 2(a)所示,在实验室中使用 DT 方法制作了一个直径 18.7 厘米、高 40 厘米的元件试样,共分五层。控制每层的质量,使其达到相对密度为 50%的中密度状态。然后,将每一层依次放入一个分模中,并使用手持夯实机仔细夯实,以达到要求的 8 厘米厚度。叶片剪切读数在试样的中心部分进行,以尽量避免尺寸和边界效应,读数频率设定为每 5 厘米一次。从图 2(b)中可以看出,叶片剪切阻力 τf 随深度的增加呈线性增长,但在 10 厘米到 20 厘米之间略呈抛物线趋势。这一现象的合理解释是,由于深度较浅,砂等颗粒材料在较低的固结应力作用下通常具有较大的有效摩擦角。然而,这种微小的偏差并不能改变这样一个结论,即如果土柱相对均匀,则土的剪切强度应随深度的增加而呈准线性增加[26]。在小型容器中,用 DT 法重组初始高度为 60 厘米的模型砂柱,以达到 Dr = 70% 的致密状态。夯实技术包括:(i) 首先在每层表面放置一块坚固的木板,(ii) 然后落下重锤使模型试样致密,如图 3(a)所示。为了得到更好的结果,改变木板的位置重复这一过程。叶片剪切试验在五个位置(中央部分和四个角落)和四个深度(10、20、30 和 40 厘米)进行。由于在同一深度获得的叶片剪切力值的分散范围很窄(即 ±15%),因此所有实验数据都取平均值。 在理想情况下,土壤容器的侧壁应(i) 在现场条件下表现得与土体完全一样,尽可能保持应力场;(ii) 在基底震动时能够进一步改变其机械特性。由于砂土液化会导致土壤刚度和模量随着过剩孔隙水压力的增加而降低[29, 30],因此上述要求通常很难满足。尽管没有完美的技术解决方案来克服上述差异,但人们对模型容器的设计已达成普遍共识。文献中已经报道了一些例子,如 (i) 等效剪力梁容器 [31] 和 (ii) 层剪力箱 [15, 16] 等。然而,就本研究关注的规模而言,这些成功应用的成本太高,无法帮助减轻边界效应,尤其是模拟液化触发后的 "零刚度 "状态。为此,首先在土壤容器(4 m × 4 m × 2 m)中按照震动方向安装了几个 20 厘米的柔性泡沫,以抑制两侧波反射的产生,如图 10 所示。随后安装厚度为 5 毫米的定制防水土工膜,以防止孔隙水渗出模型试样。如图 11(a)所示,在沉积砂粒之前,在底部放置了一层由砾石组成的排水层,作为宏观的 "多孔石"。采用 DT 方法制作了一个 Dr 值约为 50%(4 层)的模型试样。两个接触层之间的界面被分解,以增加它们之间的内聚力。对于如此重的质量,用高频率的基础振动来对模型试样进行压实超出了现有设备的能力范围;因此,采用了动态压实机来代替人工压实。然后开始采用与小容器中相同的饱和技术(图 11(b))。如图 12 所示,本研究使用正弦波(地面加速度峰值 = 0.4 g,加载频率 f = 2 Hz)作为基础激励。输入运动在 5 至 20 秒之间进行梯形校正,以提高伺服系统的波形再现性。此外,虽然由于高压油的共振,振动台确实会出现一些轻微的运动,但在开始和结束时都分配了两个各约 5 秒钟的无运动安全时间间隔。在重组过程中,在模型试样中埋设了三个孔隙水传感器阵列(L = 左侧、ML = 左侧中部和 C = 中央),以捕捉液化演变过程。详细的仪器平面图见图 13(b)。图 14 显示了三个不同深度的过剩孔隙水压力 (EPWP) Δu 的时间历程。图中灰色不连续线表示液化的触发。在图 14(c)的底部,三条曲线几乎相互重叠。这表明底部的土壤元素经历了几乎相同的加载历史,其响应没有受到边界效应的影响。至于图 14(b)的中间部分,位于中心的曲线与位于 ML 的曲线接近。然而,它们与左角的曲线明显不同,这与底部观察到的情况相反。在图 14(a)中的顶部自由表面附近,也可以得出类似的结论。中心附近和中心处的两条曲线(C 和 ML)几乎遵循相同的趋势,与左角附近的曲线明显不同。上述现象表明,底部的边界效应非常微弱,可以忽略不计。随着深度的减小,边界效应发挥了更重要的作用,尤其是在顶部自由表面附近。这与之前文献[15, 16, 32]的结果一致。更重要的是,由于附着的柔性泡沫可以适当减少侧壁的波反射,从而保证液化分析所需的简单剪切条件,因此模型试样中心周围约一半的区域不受边界效应的影响。基底震动后,孔隙水压力立即开始消散。图 14 显示,在 t = 60 秒时,EPWP 几乎消散,ru 接近 0。 这意味着在随后的叶片剪切试验中,EPWP 消散只是次要的,尤其是在设备准备阶段持续约 1 小时之后。图 16 显示了叶片剪切读数与深度之间的关系。从图中可以看出,模型试样三分之二部分的剪切强度损失最为严重。这一现象可由以下两个独立因素解释。首先,模型试件的三分之二部分与顶部的自由排水面之间有一段距离。这无疑增强了排水状态,有利于过剩孔隙水压力 Δu 的积累。其次,该部分的覆盖层有效应力不如底层高。因此,Δu 的适度增加就足以引发砂土液化。本研究制造了两个土壤容器,以开发用于砂土液化分析的大型振动台试验。第一个容器较小,目的是寻求合适的重组和饱和方法。第二个容器很大,目的是以几乎实际的工程尺寸探索砂土液化。我们可以从获得的结果中得出以下结论:DT 方法有利于制作模型试样,因为它通常
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引用次数: 0
Quantitative Elimination of Seismic Pseudofaults and Fine Analysis of True Faults Underlying Igneous Rocks of No-Well Areas: A Case Study of Shuntuoguole Uplift in Tarim Basin 无井地区火成岩下地震伪断层的定量消除和真断层的精细分析:塔里木盆地顺图郭勒隆起案例研究
IF 2.4 4区 地球科学 Q3 GEOCHEMISTRY & GEOPHYSICS Pub Date : 2024-04-30 DOI: 10.2113/2024/lithosphere_2023_129
Ziran Jiang, Jian Jiao, Qiaomu Qi, Xingyu Deng
After multistage tectonic movement and evolution, large superimposed oil and gas basins generally developed many igneous rocks in the early rifting stages. The lithology and lithofacies of igneous rocks are complex, which is easy to lead to the distortion of the underlying migration velocity field and thus the response of seismic pseudofaults. Also, because of the obvious shielding and absorption effect of igneous rocks on seismic waves, the waveform quality of underlying strata is poor and the seismic response characteristics of faults are fuzzy. Currently, relevant studies have shown that the influence of igneous rock can be eliminated by the prestack depth migration with an accurate igneous rock velocity model. However, improving the accuracy of the velocity model needs to be corrected by well-logging data, resulting in poor applicability of the existing velocity modeling technology underlying igneous rocks without well, which is an obvious technical bottleneck. In this paper, the secondary strike-slip fault in Shuntuoguole low uplift of Tarim Basin, which has great oil and gas exploration potential but a very low degree of drilling, is selected as the research object. Aiming at difficult fault detection underlying igneous rocks caused by lack of drilling, the accuracy of fault seismic identification is improved by “interpretative fault preprocessing” and “fault sensitive attribute optimization.” In addition, through the “extreme hypothesis method” to maximize the complex migration velocity and simulate the underlying target layer distortion maximization, we realize the quantitative elimination of seismic pseudofaults. The practical application shows that this technology can determine the true and fake underlying faults quantitatively without establishing an accurate igneous rock velocity model. It is crucial not only for exploring oil and gas in the Tarim Basin’s secondary strike-slip faults but also for offering a method and technical guide for identifying faults in other basins affected by igneous rocks.Large superimposed oil and gas basins have undergone multiple periods of tectonic movement and evolution and generally experienced multiple periods of strong magmatic activity in the early stages of rifts or rifts, preserving numerous igneous rocks. As a high-velocity rock mass, igneous rock has two major impacts on the precise structural imaging of its underlying strata [1]. First, igneous rocks strongly shield and absorb seismic waves, leading to the blurring of seismic response characteristics of small structures and faults in the underlying strata. Second, the uneven distribution of thickness, the lateral and vertical variability of lithology, and the significant velocity differences between different lithologies of igneous rock bodies make it difficult to accurately describe the areal distribution, thickness, and velocity of high-velocity igneous rocks before migration imaging. This reduces the accuracy of the migration velocity field a
本文使用地震属性进行断层探测。大量实验发现,特征值一致性属性对大尺度断层敏感,曲率属性对中尺度断层敏感,自动断层提取(AFE)和似然性对小尺度断层敏感[30]。图 3 显示了不同阶段数据处理后的断层分布特征。与其他图相比,图 3(c) 对不同尺度的故障(图 3(a))进行了更清晰的描述,并显著降低了噪声(图 3(b))。从图 3(c)可以看出,大尺度断层(黄色箭头)的平面分布及其断裂边缘更加清晰,中尺度断层(粉色箭头)的平面连续性更好,小尺度断层(白色箭头)的数量明显增加。显然,所提出的断层精细预测技术能有效解决火成岩下地震断层的模糊响应特征问题。根据断层多属性融合图,对奥陶系目标层进行了平面和剖面精细断层解释,共识别出 65 条断层(图 3(d))。需要注意的是,为了提高预测精度,对原始地震数据量进行了断层增量,在突出真断层的同时,也增强了伪断层的地震响应。根据顺图郭勒隆起区二叠系火成岩的地震地质特征(图 4(a)),设计了正演模型并开展了正演模型研究。正演模型中间为高速度的英安岩,两侧为低速度的火成岩,因此模型水平方向存在岩性和速度的突变(图 4(b))。在正演建模中,采用与辉绿岩速度相近或比辉绿岩速度更低、更平滑的速度作为辉绿岩层的迁移速度,在速度突变点出现断层错动,与实际地震剖面上的断层非常相似。这证实了高速火成岩的迁移速度误差是火成岩下层产生假断层的原因(图 4(c))。此外,岩性与速度的突变点,即地层中高速火成岩厚度的突变点,也是地震伪断层的位置。众所周知,在油气勘探的早期阶段,提高火成岩的速度建模精度与降低钻井风险本质上是矛盾的。对于前者,必须首先通过钻井获得先验信息(如测井数据),以约束和校正背景速度场。对于后者,必须进行高精度速度建模,以获得精确的迁移成像数据,从而对断层和构造进行精细解释。这两项工作不可避免地要先后进行,而不能同时完成,这也是现有火成岩速度建模技术在无井地区应用的瓶颈。根据对顺图郭勒隆起主要走向-滑动断层中钻孔火成岩岩层间的岩性速度分析,认为虽然无法准确求解无井约束下高速火成岩的迁移误差真实值,但可以通过 "极端假设法 "估算迁移速度误差的范围和最大值。极限假设是一种基于数学最大化概念的技术,即在假设的极限状态下对复杂问题进行分析,使问题简单化、极端化、简明化[31]。火成岩成因复杂,岩性多样。特别是喷出面的火成岩,是岩浆沿地表流动后,在喷发及其重力的作用下逐渐凝结形成的。与爆炸面和火山沉积岩相比,喷出面的火成岩具有较高的间隔速度和较简单的岩性[32]。因此,在研究区域的不同地点,喷出面火成岩的区间速度相对稳定(表 1)。利用原始地震资料得出的高速火成岩背景速度和区域喷出面高速火成岩的区间速度,估算出迁移速度误差范围,进而确定最大误差值。
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引用次数: 0
Method for Pressure Relief in Deep Coal Mine Roadways Using Borehole Groups and Its Application to Guqiao Coal Mine 利用钻孔群对深部煤矿巷道进行降压的方法及其在顾桥煤矿的应用
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-04-30 DOI: 10.2113/2024/lithosphere_2023_354
Yinyu Li, Li Qing, Yongshui Kang, Rui Zhang, Xiang Li, Bin Liu, Zhi Geng
With the increase in the mining depth of coal mines in China, the problem of large deformation of roadways owing to high-ground pressure has become prominent even under enhanced support systems. To reduce the high pressure on the surrounding rock, this study investigates a pressure-relief method for deep roadways using drilling borehole groups. Based on a deep roadway in the Huainan mining area of China, the influences of drilling parameters, such as borehole diameter, length, and arrangement were investigated. The results indicate that the fan-shaped arrangement of the borehole group can compensate for the dilatancy deformation of the surrounding rock. The peak stress of the surrounding rock is reduced and transferred to the inner part of the surrounding rock. Furthermore, a field experiment was conducted on an experimental roadway. The deformation of the roadway was monitored and compared with that of an adjacent roadway that did not apply the pressure-relief method. The monitoring results indicated that the deformation of the experimental roadway was significantly reduced.In China, coal is a major energy resource, which plays a dominant role in energy systems. China’s coal reserves are approximately 597 trillion tons, out of which approximately 53% are buried in the deep stratum (exceeding the depth of 1000 m) [1-3]. With the increase in the coal mining depth in recent years, an increasing number of roadways suffer from high geo-stress, which induces large deformation and failure and poses serious threats to mining safety [4-6]. Therefore, preventing large deformations of deep roadways with high geo-stress has become an important issue in coal mining. To prevent large deformation problems in deep roadways, engineers usually enhance the support system. For example, the use of high-strength and super-long bolts [6, 7], a method of bolting and shotcreting, U-steel support, grouting and floor bolting casting [3-5], and the reduction of the interval spacing of the supporting structures [4, 5]. Although some development has been achieved, large roadway deformations still frequently occur under high-ground pressure. The resistance offered by the supporting structure is extremely limited. Repeated repair is difficult and results in significant economic losses. Another approach to prevent large deformations of roadways is to release the high-ground pressure around the roadway using special measures. For example, floor grooving releases the high stress that accumulates on the floor, which is conducive to treating floor heaves [7, 8]. The rock mass within the range of pressure relief is destroyed by using high-pressure water injection softening and blasting pressure-relief methods, which reduces the elastic modulus and strength of the rock mass [5-7]. Drilling boreholes [6-9] in coal seams is beneficial for preventing coal and gas outburst accidents. Consequently, the accumulated energy on the surrounding rock surface decreases, leading to the release of
[20]通过建立模型实验,研究了深部巷道中钻孔直径对围岩力学性能的影响,并获得了合理孔距值的计算公式。Mishra 等人[21]提出了一种现场监测的钻孔泄压方法,用于评估单孔开挖巷道。Liu 等人[22]利用数值模拟分析了不同钻孔布置对围岩结构的破坏和高应力传递。Lan 等人[23]和 Guo 等人[24]模拟分析了钻孔直径、钻孔间距和煤应力对卸压的影响。Ma等人[25]和Song等人[26]都研究了巷道降压孔与螺栓的联合支护机理。然而,很少有研究关注深部煤矿巷道利用钻孔群降压方法的现场实验[27-29]。本研究通过数值模拟和现场实验研究了钻孔群对深部巷道稳定性的影响。提出了一种扇形钻孔组布置方式。此外,还在实验巷道上进行了应用实验。淮南矿区顾桥煤矿位于中国安徽省(见图 1)。淮南矿区顾桥煤矿位于中国安徽(见图 1),设计年生产能力为 1000 万吨。东翼巷道埋深超过 1000 米,原位应力测试最大值约为 32 兆帕。岩体主要由泥岩、砂质泥岩、粉砂岩和煤层等软岩组成。因此,尽管采用了加强支护方法,巷道仍经常出现巨大变形。严重的底板隆起和顶板下陷经常发生,需要反复维修。本研究选择了一条东翼带状巷道作为利用钻孔组进行降压方法的实验巷道。实验段长约 60 米(见图 2)。试验巷道上覆煤层 11-2,下伏煤层 8,11-2 煤层和 8 煤层无开采活动。该段上覆煤层 11-2 和下伏煤层 8 倾角较缓,煤层倾角约为∠2-4°。水文地质条件简单,主要水害为砂岩裂隙水,正常来水量为1-3 m³/h。监测点1#、2#布置在实验巷道内,监测点A1#、A2#布置在铁路巷道内,与皮带巷道相邻,不实施降压方案(见图2),地质条件和支护系统相似。开挖方法采用人工空气锤钻孔分层爆破法。巷道断面宽 5.6 米,高 4.6 米。岩层主要由砂质泥岩、粉砂岩和细粉砂岩组成。岩层倾角约为 3-8°。之前开挖的地质条件类似的巷道,虽然采用了加强支护方法,但巷道表面变形严重,开挖后 3 个月内巷道表面最大位移超过 500 毫米(见图 3)。假定泄压后,开挖引起的峰值应力会降低,促进高应力向围岩的深层传递,降低围岩发生大变形和破坏的风险。利用弹塑性力学理论建立了钻孔力学模型(见图 5)。为便于分析,假定这是一个平面应变问题。使用极坐标系是为了简化钻孔内壁抵抗均匀分布的径向应力 P1 的变形能力。应力平衡方程可表示为 [30, 31]:其中,σr 和 σθ 分别代表径向应力和圆周应力,r 为极坐标半径。 在降压应力和时间效应的影响下,钻孔壁岩体会发生坍塌,堵塞钻孔[23]。对实际钻孔坍塌条件的研究表明,钻孔形成后,原岩层中会形成孔洞效应,导致钻孔周围应力重新分布。岩层的原始应力有平衡和不平衡之分。沿钻孔中心轴线的周围岩体可分为四个区:破碎区、塑性区、弹塑性区和弹性区。在钻进过程中,钻具会扰动井壁周围的岩石,从而形成断裂带,岩石大多呈块状分布。由于钻孔的降压作用,周围的断裂发展成最不稳定的状态。由于巷道围岩的应力和时间的影响,断裂区域的岩体可能会发生崩落或坍塌,导致钻孔堵塞和堵塞。总之,在围岩中钻孔会形成一个降压区,破坏原岩层的应力平衡,重新分配钻孔周围的应力。钻孔过程会破坏岩体,降低岩体强度,导致孔周围出现裂缝。这会导致破碎区煤体和岩体稳定性变差,孔壁岩体坍塌,在卸压应力作用下堵塞孔口,最终达到消耗应力的目的。指定角度钻孔的目的是降低纵向应力集中区的应力,方便钻机施工。通过数值模拟和现场实验,研究了钻孔组对深部巷道稳定性的影响。通过数值模拟和现场实验,研究了钻孔组对深部巷道稳定性的影响,提出了一种扇形布置的钻孔组,并将其应用于顾桥煤矿的实验巷道。主要结论如下:高应力与低强度之间的矛盾是深部巷道产生较大变形的关键原因。数值模拟和现场监测结果表明,合理的钻孔降压措施能有效降低巷道围岩的高应力。数值模拟和现场试验结果表明,本研究提出的降压钻孔设计方案能有效减缓巷道大变形速率,降低巷道围岩变形。现场对比监测结果表明,两侧围岩变形可减少约 35.53%,顶板下垂可减少约 33.19%,底板隆起可减少约 35.85%。合理的钻孔卸压可有效降低集中应力,可作为防治深部高应力软弱围岩大变形灾害的辅助手段。数值模拟和现场监测结果表明,合理的钻孔降压措施可有效降低巷道围岩的高应力。现场对比监测结果表明,两侧围岩变形可减少约 35.53%,顶板下垂可减少约 33.19%,底板隆起可减少约 35.85%。合理的钻孔卸压可有效降低集中应力,可作为防治深部高应力软弱围岩大变形灾害的辅助手段。我们感谢淮南矿业(集团)有限责任公司在数据收集和岩石观测方面提供的支持。钻孔塑性区半径方程的推导见补充材料。文件中给出了钻孔轴向应力和轴向应变的表达式。确定了钻孔周围的应力边界条件。然后推导出 σθ、σr 和 σL 的表达式。钻孔临界屈服应力公式是通过获得钻孔周围应力公式并结合相关的 Tresca 屈服准则得出的。
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引用次数: 0
Optimal Inversion Method Based on Joint Waveform Inversion and Least Squares Reverse Time Migration 基于联合波形反演和最小二乘反向时间迁移的最佳反演方法
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-04-30 DOI: 10.2113/2024/lithosphere_2023_361
Kai Zhang, Yipeng Xu, Zhenchun Li, Zilin He, Yiming Pan
Joint Waveform inversion (JWI) uses the results of reflection waveform inversion (RWI) as the initial model for full waveform inversion (FWI). Compared with the FWI, the JWI method can obtain more information about the structure of the subsurface medium. The reason is that the reflected waveform inversion can invert the long wavelength component in the middle and deep areas. In JWI, reflected waveform inversion is used to obtain the reflected wave information in the simulation record by demigration, which is computationally more expensive than FWI; the least squares reverse time migration (LSRTM) also obtains the reflected wave information in the simulated record by demigration. In order to effectively use the reflected wave information brought by the high computational amount of reverse migration in JWI, this paper proposes a simultaneous inversion method of JWI and LSRTM (JWI-LSRTM). This method can simultaneously perform an iterative update of the subsurface medium velocity of JWI and the migration imaging of LSRTM, which improves the calculation data utilization rate of each forward and inversion process. In the model test, the effectiveness of the method is proved.Reflected waveform inversion (RWI) is a technique that obtains reflected wave information from simulated records through reverse migration. It can invert long wavelength components in the middle and deep layers [1-3], but its computational cost is higher than full waveform inversion (FWI). FWI is a high-precision inversion method [4-6] with the potential to provide accurate models of subsurface media parameters. Joint waveform inversion (JWI) [7] leverages the results of reflection waveform inversion (RWI) as an initial model for FWI. Compared to FWI, JWI can retrieve more information about the subsurface media structure [8]. This is because RWI can obtain long wavelength components in the middle and deep layers [9, 10]. Ren (2019) proposed an adaptive JWI method that automatically switches between RWI and FWI by adjusting the weight factor with the number of iterations and allowable errors, without manually pausing the switch [11]. This approach addresses the limitations of traditional waveform inversion methods and improves the efficiency and accuracy of subsurface media modeling.The LSRTM [12, 13] is based on the Born approximation, and the reflection coefficient is solved by many iterations with the known background velocity. LSRTM is also used to obtain the reflected wave information from simulated records.In the above three methods, the simulated data and observed data are inverted using the generalized least squares method to obtain the corresponding gradient. However, the computational cost of forward modeling the wave equation and reverse migration is substantial, accounting for at least 90% of the total computation time in these three methods. As a result, the inversion cycle is often prolonged [14, 15]. Now there are a variety of programming techniques (MPI, Openmp, Open
联合波形反演(JWI)将反射波形反演(RWI)的结果作为全波形反演(FWI)的初始模型。与全波形反演相比,联合波形反演方法可以获得更多有关地下介质结构的信息。这是因为反射波形反演可以反演中深部的长波长分量。在 JWI 中,反射波形反演是通过反演来获取模拟记录中的反射波信息,其计算成本比 FWI 高;最小二乘反向时间迁移(LSRTM)也是通过反演来获取模拟记录中的反射波信息。为了有效利用 JWI 反演计算量大带来的反射波信息,本文提出了一种 JWI 和 LSRTM(JWI-LSRTM)同步反演方法。该方法可同时对 JWI 的地下介质速度和 LSRTM 的迁移成像进行迭代更新,提高了各正演和反演过程的计算数据利用率。反射波反演(RWI)是一种通过反向迁移从模拟记录中获取反射波信息的技术。它可以反演中深层的长波长成分[1-3],但其计算成本高于全波形反演(FWI)。全波形反演是一种高精度反演方法[4-6],有可能提供地下介质参数的精确模型。联合波形反演(JWI)[7] 利用反射波形反演(RWI)的结果作为 FWI 的初始模型。与 FWI 相比,JWI 可以获取更多有关地下介质结构的信息[8]。这是因为 RWI 可以获得中深层的长波长成分[9, 10]。Ren(2019)提出了一种自适应 JWI 方法,该方法通过调整权重系数,根据迭代次数和允许误差在 RWI 和 FWI 之间自动切换,无需手动暂停切换[11]。这种方法解决了传统波形反演方法的局限性,提高了地下介质建模的效率和精度。LSRTM[12, 13]基于 Born 近似,在已知背景速度的情况下,通过多次迭代求解反射系数。上述三种方法都是利用广义最小二乘法对模拟数据和观测数据进行反演,得到相应的梯度。然而,波方程正向建模和反向迁移的计算成本很高,至少占这三种方法总计算时间的 90%。因此,反演周期往往会延长[14, 15]。现在有多种编程技术(MPI、Openmp、Openacc、GPU)或优化方法(L-BFGS 法、伪牛顿方向校正混合共轭梯度法等)可以缩短这一周期,还有一些方法可以提高计算数据的利用率(FWI 成像、RWI 和 LSRTM 联合反演)[16, 17]。为了更有效地利用 JWI 高计算解译带来的反射波信息和波方程正演模拟数据,本文提出了一种 JWI 和 LSRTM 同步反演方法。该方法可以同时更新 JWI 中地下介质的速度和 LSRTM 的迁移剖面,提高了计算数据在正演和反演过程中的利用率。本文以较容易实现的声学为例,通过模型试验和噪声数据证明了所提方法的有效性。以下是声波的波方程和反演方程:其中 x 和 z 为空间坐标,t 为时间,p0 为背景场,p 为干扰场,vp 为 p 波速度。式(2)中,dcalxr,t;xs 为模拟数据,dcalrefxr,t;xs 为散射数据,dobsxr,t;xs 为观测数据,m 为反射系数,其表达式为:mimage(x)=Δv(x)vp(x),散射数据可通过式(2)计算。其邻接方程和梯度公式可通过邻接法获得。其中,T 为最大记录时间 dcal,m 为次表层介质参数,分别为模拟数据(由方程 dobs(1) 求得)和观测数据。
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引用次数: 0
Influence of Rock Fabric on Physical Properties of Shale Oil Reservoir Under Effective Pressure Conditions 有效压力条件下岩石结构对页岩油藏物理性质的影响
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-04-30 DOI: 10.2113/2024/lithosphere_2023_338
Yu Ma, Suping Yao, Ning Zhu, Huimin Liu, Junliang Li, Weiqing Wang
The physical properties of shale oil reservoirs under overburden pressure are of great significance for reservoir prediction and evaluation during exploration and development. Based on core, thin section, and SEM observations, as well as test data such as XRD, TOC, and porosity and permeability under pressure conditions, this study systematically analyzes the variation of physical properties of different lithofacies shales in the Jiyang depression and the influence of rock fabric on the physical variation under pressure. The porosity and permeability of shale samples significantly decrease under pressure. According to the phased reduction in porosity and permeability, the pressurization process is divided into three pressure stages: low pressure (<8 MPa), medium pressure (8–15 MPa), and high pressure (>15 MPa). The reduction of porosity is fastest in the low-pressure stage and slowest in the medium-pressure stage. The reduction of permeability is fastest in the low-pressure stage and the slowest in the high-pressure stage. The rock fabric has a significant impact on porosity and permeability under pressure conditions. The permeability of laminated shale and bedded shale is higher than that of massive shale under pressure, and the permeability loss rate is lower than that of massive shales. Especially under lower pressure, the difference can be 10–20 times. In addition, the reduction rate of porosity and permeability under pressure is negatively correlated with felsic minerals content, which is positively correlated with carbonate minerals content and clay minerals content. The contribution of clay minerals to the porosity reduction rate is dominant, followed by carbonate minerals. The contribution of carbonate minerals to the permeability reduction rate is dominant, followed by clay minerals. The TOC content has no significant impact on the porosity and permeability of shales under pressure in the study due to the low maturity.With the change in global energy structure, shale oil and gas has become the core growth point of China’s oil and gas resources [1-4]. In the past decade, a series of important progresses have been made in the exploration and development of shale oil and gas in China, including breakthroughs in the exploration of shale oil in Junggar Basin, Ordos Basin, Jianghan Basin, Songliao Basin, and Bohai Bay Basin [5-8]. However, due to the heterogeneity of shales and the complexity of geological conditions in China, the prediction and evaluation of shale oil reservoirs still face many challenges [3, 9, 10].Many studies have shown that rock fabric, such as laminated structure and mineral composition, has a significant influence on the pore development and physical properties of shale oil reservoirs [10-14]. However, most of these studies were conducted under unpressurized conditions, and there are some errors with the formation conditions, which affect the prediction and evaluation of shale oil desserts. To recover the real physical
页岩油藏在覆盖层压力下的物性对于勘探和开发过程中的储层预测和评价具有重要意义。本研究基于岩心、薄片和扫描电镜观察,以及XRD、TOC、压力条件下孔隙度和渗透率等测试数据,系统分析了济阳凹陷不同岩性页岩的物性变化,以及岩石结构对压力作用下物性变化的影响。在压力作用下,页岩样品的孔隙度和渗透率明显降低。根据孔隙度和渗透率的阶段性降低,加压过程分为三个压力阶段:低压(15 兆帕)。孔隙度在低压阶段降低最快,在中压阶段降低最慢。渗透率的降低在低压阶段最快,在高压阶段最慢。在压力条件下,岩石结构对孔隙度和渗透率有很大影响。在压力作用下,层状页岩和层状页岩的渗透率高于块状页岩,而渗透率损失率低于块状页岩。特别是在低压条件下,两者相差可达 10-20 倍。此外,压力下孔隙度和渗透率的降低率与长石矿物含量呈负相关,与碳酸盐矿物含量和粘土矿物含量呈正相关。粘土矿物对孔隙度降低率的贡献占主导地位,碳酸盐矿物次之。碳酸盐矿物对渗透率降低率的贡献最大,其次是粘土矿物。随着全球能源结构的变化,页岩油气已成为我国油气资源的核心增长点[1-4]。近十年来,我国页岩油气勘探开发取得了一系列重要进展,包括准噶尔盆地、鄂尔多斯盆地、江汉盆地、松辽盆地、渤海湾盆地等页岩油勘探取得突破[5-8]。然而,由于页岩的异质性和中国地质条件的复杂性,页岩油藏的预测和评价仍面临许多挑战[3, 9, 10]。许多研究表明,层状构造和矿物组成等岩石结构对页岩油藏的孔隙发育和物性有重要影响[10-14]。然而,这些研究大多是在无压条件下进行的,与地层条件存在一定误差,影响了页岩油甜点的预测和评价。为了恢复地层条件下的真实物理参数,一些学者进行了加压实验,发现页岩的孔隙度和渗透率都随着有效压力的增加而逐渐降低,并提出了指数函数、二项式等函数模型来描述加压过程中孔隙度和渗透率随压力的变化[15-22]。然而,对于单个页岩样本而言,在相同压力条件下,不同样本之间的孔隙度和渗透率差异较大[17-19],造成这些差异的原因尚不清楚,有待进一步探讨。本研究选取了济阳凹陷的 Es3x-Es4s 页岩。通过岩石学、矿物学、有效压力下的孔隙度和渗透率实验以及 FE-SEM 观察,探讨了有效压力下页岩储层的物理特征以及岩石结构对孔隙度和渗透率的影响,为预测和评价济阳凹陷古新统页岩油藏提供依据。济阳凹陷位于中国渤海湾盆地东南部,由南向北依次为东营、惠民、沾化和车镇四个子凹陷(图 1(a))[23]。在近十年的勘探中,东营、沾化等子凹陷多层次、多类型页岩油取得重大突破,显示出济阳凹陷页岩油良好的勘探前景[24-26]。目前,Es4s、Es3x 和 Es1 是济阳凹陷页岩油的主要勘探区间(图 1(b)),其特点是碳酸盐岩含量高,平均含量超过 50%[23、27、28]。作为济阳凹陷页岩油的主要勘探区带,Es4-Es3x有许多工业油流井和采样井。 本研究的样品采集自 BYP5 井、F201 井和 FYP1 井(图 1(a)),基本信息见表 1。首先,从岩心样品中钻出一个与基底平行的塞状样品(直径 25 毫米,长 60 毫米)。然后,从塞子的一侧切割出一个 2 厘米高的微型塞子,用于薄片和扫描电子显微镜观察。剩余的塞子样品用于测量有效压力下的孔隙度和渗透率。在完成孔隙度和渗透率测量后,将塞子样品粉碎,用于总有机碳和矿物成分分析。使用蔡司显微镜观察厚度为 30 μm 的岩石薄片,以明确层理的发育特征和矿物分布。使用高分辨率场发射扫描电子显微镜(蔡司 Sigma 500)观察孔隙的形态、大小和分布。使用配备 J&M MSP200 显微光度计的蔡司显微镜对样品表面(10 × 10 μm)进行手工研磨和氩离子抛光(Leica EM 3X),以获得更好的图像质量。总有机碳 (TOC) 含量是用 Vario MICRO 立方体元素分析仪测定的。测试前,将页岩样本研磨至小于 200 目,并与稀 HCL 反应 72 小时以去除碳酸盐矿物。X 射线衍射(XRD)分析是使用 Dmax IIIa 衍射仪和铜 X 射线管(40 千伏,30 毫安)进行的。粘土矿物的分离和 XRD 测试按照中国石油行业标准(SY/T 5163-2018)进行。上述实验在南京大学表层地球化学教育部重点实验室进行,有效压力条件下的孔隙度和渗透率采用 PoroPerm-200 全自动孔隙度-渗透率仪进行测量。超压条件的实现主要依靠岩心保持系统,该系统以气体为加压介质,模拟水力压裂加压,从而实现超压条件下孔隙渗透率的在线测试。实验过程中,加压气源采用高压空气,测试采用高纯度氦气。为避免滑移效应对页岩样本渗透率的影响,在加压过程中保持驱动压力恒定。实验中设定的有效压力点在加压过程中保持不变。实验中设定的有效压力点分别为 2.41、4.48、6.55、8.62、10.69、12.07、20、30 和 50 兆帕。在每个压力点保持测量 30 分钟,稳定后测量相应压力下的孔隙度和渗透率。过压实验前,页岩样品需要用二氯甲烷和甲醇(93:7)萃取(72 小时),以去除样品中的残余油。根据层理厚度,结合岩芯和薄片观察,将页岩样品划分为层理页岩(2 厘米)。除块状页岩外,层状页岩和层状页岩的层理均较发育,表现为浅色层理和深色层理交替出现(图 3)。浅色层理的主要矿物为方解石,泥晶方解石和疏松方解石之间漂浮着少量石英、长石和白云石;深色层理的矿物成分较为复杂,以粘土矿物为主,还含有一些方解石、白云石、石英、长石和有机质(OM)。层状矿物成分的不同导致层状页岩和层状页岩中矿物分布的强烈异质性。表 2 列出了页岩样本的平均玻璃光泽反射率(Ro%)、总有机碳含量和矿物成分。本研究中的页岩样本热成熟度较低(0.78% Ro 至 1.12% Ro),总有机碳含量适中(2.85% 至 6.26 wt%,平均 3.51 wt%)。矿物包括方解石(7-69 wt%,平均 37 wt%)、粘土矿物(4-30 wt%,平均 22%)、石英(10-34 wt%,平均 19 wt%)、长石(4-22 wt%,平均 11 wt%)、白云石(3-22 wt%,平均 10 wt%)和少量黄铁矿(1-3 wt%,平均 15 MPa)。
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引用次数: 0
Formation of the Great Bend and Enhanced Quaternary Incision of the Upper Yangtze River: New Insights from Low-Temperature Thermochronology and Tributary Morphology 长江上游大拐弯的形成与第四纪侵蚀作用的增强:低温热时学及支流形态学的新见解
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-03-25 DOI: 10.2113/2023/lithosphere_2023_244
Yong Zheng, J. Pan, Haibing Li, Yang Wang, Zheng Gong, M. Bai
The occurrence of a sharp turn along the upper course of the Yangtze River is referred to as the “Great Bend” and represents a large-scale drainage reorganization in response to the surface rise of the Tibetan Plateau. However, the timing and mechanism of the formation of the Great Bend remain disputed. In this paper, we report new (U–Th)/He and apatite fission track thermochronological data from the deep river valley in the Great Bend area of the southeastern margin of the Tibetan Plateau. Compared with the adjacent Jianchuan Basin, two phases of younger rapid cooling for the Great Bend area are identified based on thermal-history modeling, namely, Miocene (ca. 17 to 11–8 Ma) and Quaternary, with the former phase being contemporaneous with the formation of the anticline in the Tiger Leaping Gorge. Progressive increases in the normalized channel steepness (ksn) and the degree of river-valley incision with increasing distance downstream for tributaries of the Yangtze River in the Tiger Leaping Gorge indicate that river rerouting and formation of the Great Bend occurred during the Miocene. Samples located at the bottom of the Tiger Leaping Gorge also reveal a phase of rapid cooling since ca. 1.9 Ma, with an exhumation rate of 1.5 ± 0.2 mm/year. We hypothesize that enhanced Quaternary exhumation in the southeastern margin of the Tibetan Plateau occurred mainly within the narrow region between the Sichuan Basin and the Eastern Himalayan Syntaxis, corresponding to an episode of widespread extensional deformation superimposed above middle- to upper-crustal flexure in this region.
长江上游出现的急转弯被称为 "大拐弯",是青藏高原地表隆起引起的大规模排水系统重组。然而,大拐弯形成的时间和机制仍存在争议。本文报告了青藏高原东南缘大拐弯地区深河谷的(U-Th)/He和磷灰石裂变轨迹热年代学新数据。与邻近的剑川盆地相比,根据热史模型确定了大拐弯地区较年轻的两个快速冷却阶段,即中新世(约17至11-8Ma)和第四纪,前一阶段与虎跳峡反斜的形成同时。虎跳峡长江支流的归一化河道陡度(ksn)和河谷切入程度随下游距离的增加而逐渐增加,表明河流改道和大拐弯的形成发生在中新世。位于虎跳峡底部的样本也显示了自约 1.9 Ma 开始的快速冷却阶段。位于虎跳峡底部的样本还显示,自约 1.9 Ma 开始,虎跳峡处于快速冷却阶段,隆升速度为 1.5 ± 0.2 mm/年。我们推测,青藏高原东南缘第四纪隆升主要发生在四川盆地与东喜马拉雅山系之间的狭长区域,与该区域中、上地壳褶皱叠加的大范围伸展变形相对应。
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引用次数: 0
Cenozoic Exhumation Across the High Plains of Southeastern Colorado from (U-Th)/He Thermochronology 从(U-Th)/He 热时学看科罗拉多东南部高原的新生代侵蚀作用
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-03-01 DOI: 10.2113/2023/lithosphere_2023_310
Sabrina J. Kainz, L. Abbott, R. Flowers, Aidan Olsson, Skye Fernandez, J. Metcalf
Colorado’s High Plains stand at anomalously high elevations (~1300–2100 m) for their continental interior setting, but when and why this region became elevated is poorly understood. The Cenozoic history of the High Plains is also likely linked with that of the Rocky Mountains, where the timing and cause(s) of uplift are similarly debated. We present apatite (U-Th)/He (AHe) data for 10 samples from Tertiary intrusives along a ~200 km west-to-east transect across the High Plains of southeastern Colorado to constrain the timing of exhumation and to gain insight into when and why regional elevation gain occurred. Mean sample AHe dates for the ~24–22 Ma East Spanish Peak pluton and associated radial dikes from the westernmost High Plains are 18.8 ± 1.4 to 14.1 ± 1.7 Ma, recording substantial postemplacement erosion. AHe results for the mafic to ultramafic Apishapa Dikes (oldest ~37 Ma, youngest ~14 Ma) located ~20–40 km farther north and east on the High Plains range from 12.0 ± 1.4 to 6.2 ± 1.9 Ma, documenting continued exhumation on the western High Plains during the ~12–5 Ma deposition of the Ogallala Formation farther east and suggesting that the western limit of Ogallala deposition was east of the Apishapa Dikes. In far southeastern Colorado, the Two Buttes lamprophyre was emplaced at 36.8 ± 0.4 Ma and yields a Late Oligocene AHe date of 27.1 ± 4 Ma. Here, the Ogallala Formation unconformably overlies Two Buttes, indicating that the regional ~12 Ma age for the base of the Ogallala is a minimum age for the exposure of the pluton at the surface. The AHe data presented here document that kilometer-scale erosion affected all of the southeastern Colorado High Plains in Oligo-Miocene time. While exhumation can have multiple possible causes, we favor contemporaneous surface uplift capable of elevating the region to modern heights.
科罗拉多高原的海拔(约 1300-2100 米)在其大陆内部环境中异常高,但人们对这一地区何时以及为何海拔升高却知之甚少。高原的新生代历史很可能与落基山脉的新生代历史有关,而落基山脉的隆起时间和原因也同样存在争议。我们展示了科罗拉多州东南部高原自西向东约 200 公里横断面上 10 个第三纪侵入体样本的磷灰石(U-Th)/氦(AHe)数据,以确定隆升的时间,并深入了解区域海拔上升的时间和原因。来自高原最西部的约 24-22 Ma 的东西班牙峰岩浆岩及相关径向岩钉的平均样品 AHe 日期为 18.8 ± 1.4 至 14.1 ± 1.7 Ma,记录了大量的置换后侵蚀。位于高原北部和东部约 20-40 公里处的黑云母至超黑云母阿皮沙帕尖峰(最古老 ~37 Ma,最年轻 ~14 Ma)的 AHe 结果为 12.0 ± 1.4 至 6.2 ± 1.9 Ma,记录了在奥加拉拉地层向东沉积的约 12-5 Ma 期间西部高原的持续剥蚀,并表明奥加拉拉沉积的西部界限在阿皮沙帕尖峰以东。在科罗拉多州的最东南部,两山灯台岩是在 36.8 ± 0.4 Ma 时沉积的,得出的晚更新世 AHe 时间为 27.1 ± 4 Ma。在这里,奥加拉拉地层不整合地覆盖在两山之上,这表明奥加拉拉地层底部的区域 ~12 Ma 年龄是该岩体露出地表的最低年龄。本文提供的 AHe 数据表明,在上新世时期,科罗拉多高原东南部所有地区都受到了千米级的侵蚀。虽然掘起可能有多种原因,但我们倾向于能够将该地区提升到现代高度的同期地表隆起。
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引用次数: 0
Advancing (U-Th)/He Zircon Dating: Novel Approaches in Sample Preparation and Uncertainty Reduction 推进(U-Th)/He 锆石定年:样品制备和减少不确定性的新方法
IF 2.4 4区 地球科学 Q2 Earth and Planetary Sciences Pub Date : 2024-02-20 DOI: 10.2113/2023/lithosphere_2023_258
Y. Hao, Ying Wang, Zhuqi Zhang, Jingxing Yu, Yizhou Wang, J. Pang, Wanfeng Zhang, Dewen Zheng
The laser microprobe (U-Th)/He dating method is a new and efficient technique that utilizes an interoperable and integrated suite of instruments, including the excimer laser system, quadrupole helium mass spectrometer, and quadrupole inductively coupled plasma mass spectrometer. To demonstrate the applicability of this new method, we applied both the conventional and laser microprobe techniques to the Sri Lanka zircon (LGC-1). We obtained twenty-two (U-Th)/He ages on nine shards using the laser microprobe method, showing an average (U-Th)/He age of 471.1 ± 16.6 Ma (1σ). This result is generally consistent with the mean conventional age (484.1 ± 9.6 Ma) for twenty-two zircon fragments. Both are nearly equal to the age value (~476 Ma) predicted by the He diffusion model and the thermal history model of Sri Lanka highland. The variations in the laser microprobe-derived ages are most likely caused by the uncertainties in volume measurements, which is also common in other studies. We used the Mahalanobis distance technique to reduce the volume measurement bias by identifying and eliminating abnormal data.
激光微探针(U-Th)/He 测年法是一种高效的新技术,它利用了一套可互操作的集成仪器,包括准分子激光系统、四极杆氦质谱仪和四极杆电感耦合等离子体质谱仪。为了证明这种新方法的适用性,我们对斯里兰卡锆石(LGC-1)采用了传统和激光微探针技术。我们利用激光微探针方法在九块碎片上获得了 22 个 (U-Th)/He 年龄,显示平均 (U-Th)/He 年龄为 471.1 ± 16.6 Ma (1σ)。这一结果与二十二块锆石碎片的平均常规年龄(484.1 ± 9.6 Ma)基本一致。两者都几乎等于斯里兰卡高地氦扩散模型和热历史模型预测的年龄值(~476 Ma)。激光微探针年龄的变化很可能是由于体积测量的不确定性造成的,这在其他研究中也很常见。我们采用了马哈拉诺比斯距离技术,通过识别和剔除异常数据来减少体积测量的偏差。
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引用次数: 0
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