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1.
本文通过岩心观察、录测井及岩心粒度资料,埘鄂尔多斯盆地麻黄山西区块北部中侏罗统延安组延一段的岩石组分、结构构造、粒度分布等特征进行分析,确定其沉积相类型。结果表明：延安组延一段属河流沉积体系,发育辫状河和曲流河两种沉积类型,主要包括河床和河漫两个亚相,可进一步识别出河床滞留、心滩、边滩、河漫滩、河漫沼泽、决口扇等微相。延一段延10油层组沉积时期,研究区以辫状河沉积为主,心滩发育,河道较宽,平面上摆动宽度为2～8km,主水流方向由西北至东南;延一段延9油层组沉积时期,受鄂尔多斯盆地湖水面整体抬升的影响,河道分布范围逐渐缩小,研究区以曲流河沉积为主,发育两条曲流河,平面上摆动宽度约2～4km,河道凸岸发育边滩沉积。 相似文献
2.
通过对研究区内12口钻井岩芯的岩石学特征、沉积构造等特征的综合认识,结合沉积微相平面展布及连井地层对比,对麻黄山西区块三叠系延长组长61油层组进行了沉积环境分析,识别出6种沉积构造,5种沉积微相,总结出6种微相接触样式.研究结果表明,延长组长61油层组为三角洲前缘沉积,垂向上表现为以反韵律为主伴有短期正韵律的沉积特征,体现了三角洲前积的过程. 相似文献
3.
通过对延长油田郭旗西区长6油层组储层的沉积微相、储层的岩石学特征、成岩作用、孔隙结构特征和物性条件研究，探讨了影响储集条件和油气成藏的主要因素.延长油田郭旗西区三叠系延长组长6早期沉积微相以三角洲前缘水下分流河道为主，长6晚期以三角洲平原分流河道沉积为主，储集层发育.受成岩后生作用影响，形成了低孔隙度、特低-超低渗透率的储集层.油藏分布主要受沉积微相和储层物性控制，为典型的岩性油藏。 相似文献
4.
鄂尔多斯盆地姬塬地区上三叠统延长组长8油层组为低孔特低渗储集层,研究该区相对优质储集层展布特征以及形成条件,并进行有利目标区域的优选和预测,对于油气挖潜具有很大的意义。通过砂岩物性、砂岩薄片及扫描电镜等资料的研究,探讨了储集层的岩石学类型、孔隙类型与物性特征、胶结物种类及成岩作用特点及其对有利储集层的控制作用。研究表明,姬塬地区长8油层组主要发育岩屑长石砂岩,铁方解石等胶结物普遍发育,储集层物性整体较差,非均质性强,主要孔隙类型为残余粒间孔和溶蚀孔隙;沉积、成岩及构造共同控制了有利储集层的分布。在此基础上,预测了姬塬地区有利储集层的分布。 相似文献
5.
《古地理学报》2017,(5)
利用岩心、铸体薄片、扫描电镜、碳氧同位素及流体包裹体等资料,对鄂尔多斯盆地姬塬西部三叠系延长组长8油层组致密储集层特征进行了研究,重点分析了储集层成岩作用特征和储集层致密化成因机制及过程。研究区长8油层组砂岩主要为岩屑长石砂岩和长石岩屑砂岩,经历了压实—压溶、胶结、交代、溶蚀及构造破裂等成岩作用,整体处于中成岩A期晚期。典型成岩序列依次为机械压实、绿泥石黏土膜、早期(泥晶)方解石胶结、石英次生加大、长石、岩屑溶蚀、自生高岭石胶结、自生石英胶结、中期(含)铁方解石胶结。综合研究认为:(1)近物源伴随湖平面快速上升的沉积环境提供了储集层致密化的物质基础,不同沉积微相储集层物性差别较大,分流河道最好,分流间湾最差;(2)长8油层组原始孔隙度为41.35%,压实作用损孔率为50.67%,造成储集层孔隙度急剧降低,胶结作用损孔率为37.48%,导致孔隙度进一步减小,溶蚀作用仅增加了3.26%的孔隙度,难以有效改善储集层质量;(3)上述沉积与成岩因素共同导致储集层致密,致密化过程可分为压实孔隙骤减阶段、早期胶结减孔阶段、溶蚀作用增孔阶段和晚期胶结致密阶段共4个阶段;(4)油气大量充注期储集层孔隙度远低于10%,长8油层组先致密后成藏。 相似文献
6.
利用岩心、铸体薄片、扫描电镜、碳氧同位素及流体包裹体等资料,对鄂尔多斯盆地姬塬西部三叠系延长组长8油层组致密储集层特征进行了研究,重点分析了储集层成岩作用特征和储集层致密化成因机制及过程。研究区长8油层组砂岩主要为岩屑长石砂岩和长石岩屑砂岩,经历了压实—压溶、胶结、交代、溶蚀及构造破裂等成岩作用,整体处于中成岩A期晚期。典型成岩序列依次为机械压实、绿泥石黏土膜、早期(泥晶)方解石胶结、石英次生加大、长石、岩屑溶蚀、自生高岭石胶结、自生石英胶结、中期(含)铁方解石胶结。综合研究认为:(1)近物源伴随湖平面快速上升的沉积环境提供了储集层致密化的物质基础,不同沉积微相储集层物性差别较大,分流河道最好,分流间湾最差;(2)长8油层组原始孔隙度为41.35%,压实作用损孔率为50.67%,造成储集层孔隙度急剧降低,胶结作用损孔率为37.48%,导致孔隙度进一步减小,溶蚀作用仅增加了3.26%的孔隙度,难以有效改善储集层质量;(3)上述沉积与成岩因素共同导致储集层致密,致密化过程可分为压实孔隙骤减阶段、早期胶结减孔阶段、溶蚀作用增孔阶段和晚期胶结致密阶段共4个阶段;(4)油气大量充注期储集层孔隙度远低于10%,长8油层组先致密后成藏。 相似文献
7.
据新的地层划分方案及大量钻井、露头和岩心资料,详细研究了鄂尔多斯盆地华池地区延安组延9油层组（Y9）沉积体系特征及演化,认为延9油层组主要为河流沉积,是延10油层组的继承与发展,发育有辫状河、辫状型曲流河和网状河3种类型的河流。Y39油层是辫状河发育的油层,Y29油层在继承Y39油层河流的基础上发育辫状型曲流河,Y19油层则是在前两期逐渐填平补齐之后,在准平原条件下发育的网状河沉积。华池地区延9油层组发育辫状河-辫状型曲流河和网状河两种河流沉积模式。 相似文献
8.
鄂尔多斯盆地湖盆中部地区三叠系延长组长6油层组中下部和长7油层组中上部大面积发育深水砂岩, 这种砂岩具有厚度大、平行于湖盆长轴方向连续分布的特征。根据沉积结构、构造及接触关系, 将深水砂岩划分为砂质碎屑流成因的砂岩、浊流成因的砂岩、滑塌成因的砂岩及三角洲前缘成因的砂岩等4种沉积类型。在储集层矿物学、岩石学特征研究的基础上, 提出深水砂岩的沉积特征(如粒度细、云母和绿泥石等塑性颗粒含量高、陆源碳酸盐岩岩屑与伊利石杂基发育等)是造成储集层抗压实能力较差、胶结强烈、储集层致密的关键因素;在有利成藏条件分析中提出深水砂岩致密储集层处于油源中心、与烃源岩互层共生是形成大面积非常规致密油资源的重要控制因素。 相似文献
9.
鄂尔多斯盆地W油田21井区低渗透储集层非均质性较强,注水开发效果不理想。为了精确描述其储集层物性及展布特征,在地质、测井和开发动态等资料的基础上,综合应用相控建模技术,针对鄂尔多斯盆地低渗透油藏采用多种建模方法相结合的手段进行了建模研究,依次建立了研究区的构造、岩相、沉积微相以及微相控制下的储层属性等相关模型。同时对油气储集层相控与非相控建模结果进行了对比,对比结果显示相控属性模型对油藏特征的描述和表征更加合理、准确,应用Petrel地质建模与Eclipse数值模拟的一体化无缝连接,使后续的CO2驱油数值模拟研究也取得了良好的应用效果。这一研究结果直接体现出相控建模技术在鄂尔多斯盆地低渗透油藏的成功应用,也预示着相控建模技术是解决多种沉积微相和非均质性较强的低渗透储集层物性参数相关模拟的有效途径,能清晰地认识和识别砂体连通性及其展布规律,可为低渗透油藏后期开发提供可靠的地质基础。 相似文献
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11.
Phase Equilibria in the System CaCO3-MgCO3-FeCO3 总被引：4，自引：0，他引：4
Experimental data on phase relations in the CaCO3-MgCO3-FeCO3ternary by Goldsmith et al. (1962) are inconsistent with thoseof Rosenberg (1967). These inconsistencies cannot be reconciledby the pressure or temperature differences between the two setsof experiments. Available reversed experiments on the binarysystems have been re-evaluated to yield consistent binary solvi.These data have been combined with analyses of natural carbonatesto yield approximate ternary phase diagrams at 250,400,550,and 700 ?C, and 4 to model ternary activity/composition relationsfor calcite- and dolomite-structure carbonates. An empiricalmodel for thermometry with calcite-ferroan dolomite was derivedfrom the ternary solvus by fitting an empirical equation tothe calcite limb of the ternary solvus. This model appears toextend reliably to higher iron contents than the models of Bickle* Powell (1977) and Powell et al. (1984). 相似文献
12.
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14.
Jianjun Liu C.-G. Duan M. M. Ossowski W. N. Mei R. W. Smith J. R. Hardy 《Physics and Chemistry of Minerals》2001,28(8):586-590
The order-disorder phase transitions in NaNO3 and CaCO3 are simulated by molecular dynamics. The simulations are based on the potentials calculated from the Gordon–Kim modified
electron gas formalism extended to molecular ions. We successfully reproduced the transition temperature T
c
and the abnormally large c axis thermal expansion observed in experiment. The phase transitions in NaNO3 and CaCO3 were found to be initiated by ±60 and ±180° reorientation of the NO3 and CO3 ions about the c axis. The orientations of NO3 and CO3 ions are continuous with six preferred calcite-type orientations above the phase-transition temperature.
Received: 30 January 2001 / Accepted: 11 May 2001 相似文献
15.
The solvus on the Mn-rich side in the system MnCO3-CaCO3 was studied experimentally at 10 kb and lower pressures. The critical point lies at 540 °C and Mn0.68Ca0.32CO3. Reaction rates of demising are extremely sluggish. X-ray calibration curves for (Mn, Ca)CO3 solid solutions are given. Depicting microprobe analyses of about 300 carbonates from manganese calc silicate marbles affected by different degrees of metamorphism confirm the experimentally derived solvus.Margules parameters were derived from the experimental solvus, giving for spinodal unmixing W
a=20.1+0.032·T and W
b=18.3-0.0033·T, and for binodal unmixing W
a=–22.9+0.035 ·T and W
b=3.36+0.0147·T (All W, in kJ/-mol)A physical interpretation of the Margules parameters based on deformations of the ionic radii in the solid solution is presented. The Margules parameters obtained by this model agree fairly well with the experimental data. 相似文献
16.
超临界流体中MoO3与WO3溶解度实验探讨 总被引：1，自引：1，他引：1
超临界地质流体以其独特的性质对金属成矿元素具有超强的萃取、层析和搬运能力,在热液矿床成矿机制研究中对揭示成矿物质的源、流和汇起着特殊和重要作用。本文利用分析纯H2MoO4在高温下脱水制备了MoO3(白色斜方晶系),在冷封式高压釜中实验测定了417℃超临界条件下,MoO3在纯水中的溶解度分别为7.3(29MPa)、14.2(45MPa)、21.6(55MPa)、27.7(78MPa)、32.5(100MPa)、和34.2(150MPa)mmol/l,热液中钼的存在形式为H2MoO4。依据前人的实验方案,补充测定了WO3在4.0%NaCl水溶液中于450%条件下的溶解度,其值分别为27.51(50MPa)和30.52(100MPa)mmol/l。结合前人研究结果发现,MoO3、WO3的溶解度在临界区域内具有超临界现象,在超临界条件下其溶解度与石英的超临界溶解度行为基本相似,表现为溶解度随体系温度和压力的升高而增大,这对揭示岩浆热液型和石英脉型钨、钼矿床的形成机制具有重要指导作用。 相似文献
17.
Polarized optical absorption spectra of Mn(IV) in octahedral crystal fields of Mn(SeO3)2 have been studied by means of microscope-spectrometry in the range 40000-4000 cm?1 and at temperatures between 113 K and 293 K. Intense charge-transfer absorptions (linear absorption coefficient α ? 30000 cm?1) completely mask the d-d transitions in the UV and VIS region above ≈23000 cm?1. The optical electronegativity χ opt of Mn(IV) in Mn(SeO3)2 is estimated to be 2.7. In accordance with the d 3 configuration of tetravalent manganese three d-d bands observed at ambient temperatures at 13250, 14137 (α≈50 cm?1) and ≈18500 cm?1 (α≈500–800 cm?1) are assigned to the spin forbidden 4 A 2g →2 E g and 4 A 2g →2 T 1g transitions as well as to the first spin allowed 4 A 2g →4 T 2g transition, respectively. These assignments allow the calculation of the following ligand field parameters: Dq ≈ 1850 cm?1, B 55 = 869 cm?1 (β 55 = 0.82), and C = 2346 cm?1 (293 K). 相似文献
18.
以安徽淮南某矿3D3C勘探施工中地面设备的实际布排为例，介绍了snake技术的应用以及其对施工效率及经济效益的影响，对如何更有效的利用该技术起到了一个抛砖引玉的作用。 相似文献
19.
Tsuneaki Goto Thomas J. Ahrens George R. Rossman 《Physics and Chemistry of Minerals》1979,4(3):253-263
Unpolarized absorption spectra of single crystals of Cr3+ doped Al2O3 (synthetic ruby) have measured using a new, time-resolving, dispersive, streak photographic system over the range ～350 to ～700 nm during a series of shock loading experiments. The crystal field absorptions assigned to the transition 4 A 2g→4 T 2g were observed to shift in a series of experiments from 555±1 nm at atmospheric pressure to 503±5 nm at 46 GPa. In a single experiment at 32 GPa the 4 A 2g→4 T 1g transition was observed to shift from 405±1 to 386±5 nm. The present data extrapolate downwards in compression toward the 10 GPa data of Stephens and Drickamer (1961) although both crystal field absorption energies increase considerably less with compression than predicted by the simple ionic point charge model. The single datum observed for the Racah parameter B, 588±38 cm?1 at 32 GPa, is consistant with previous results to 10 GPa and the trend of decreasing B, with compression expected from the divergence of the data from the point charge model due to increasing covalancy. 相似文献
20.
Enthalpies of drop solution (ΔH
drop-sol) of CaGeO3, Ca(Si0.1Ge0.9)O3, Ca(Si0.2Ge0.8)O3, Ca(Si0.3Ge0.7)O3 perovskite solid solutions and CaSiO3 wollastonite were measured by high-temperature calorimetry using molten 2PbO · B2O3 solvent at 974 K. The obtained values were extrapolated linearly to the CaSiO3 end member to give ΔH
drop-sol of CaSiO3 perovskite of 0.2 ± 4.4 kJ mol−1. The difference in ΔH
drop-sol between CaSiO3, wollastonite, and perovskite gives a transformation enthalpy (wo → pv) of 104.4 ± 4.4 kJ mol−1. The formation enthalpy of CaSiO3 perovskite was determined as 14.8 ± 4.4 kJ mol−1 from lime + quartz or −22.2 ± 4.5 kJ mol−1 from lime + stishovite. A comparison of lattice energies among A2+B4+O3 perovskites suggests that amorphization during decompression may be due to the destabilizing effect on CaSiO3 perovskite from a large nonelectrostatic energy (repulsion energy) at atmospheric pressure. By using the formation enthalpy
for CaSiO3 perovskite, phase boundaries between β-Ca2SiO4 + CaSi2O5 and CaSiO3 perovskite were calculated thermodynamically utilizing two different reference points [where ΔG(P,T )=0] as the measured phase boundary. The calculations suggest that the phase equilibrium boundary occurs between 11.5 and
12.5 GPa around 1500 K. Its slope is still not well constrained.
Received: 20 September 2000 / Accepted: 17 January 2001 相似文献