苏里格气田苏14井区盒8段层序地层格架中的沉积微相与砂体分布规律研究

鄂尔多斯盆地苏里格气田苏14井区上二叠统盒8段沉积特征与4个中期基准面旋回密切相关,盒8下亚段的MSC1、MSC2中期旋回主要发育基准面上升半旋回,为辫状河沉积;盒8上亚段2小层的MSC3旋回东部为上升半旋回,西部为非对称旋回,沉积相呈"东辫西曲"的格局;盒8上亚段1小层的MSC4旋回为对称旋回,主要发育曲流河沉积。这种沉积格局进而影响砂体分布,MSC1旋回和MSC2旋回砂体规模大,厚度大,横向连续性好;MSC3旋回东部砂体规模较西部大,横向连续性较好;MSC4砂体规模减小,厚度较薄,多呈孤立状,横向连续性差。     

苏里格气田苏14 井区盒8 段河流相砂体展布与演化规律研究

河流相砂体横向相变快,连续性和连通性差,储层非均质性强,严重影响了河流相储层的开发效果。依据储层沉积学的研究方法,对苏里格气田苏 14 井区盒 8 段河流相砂体展布与演化规律进行了研究。结果表明：苏 14 井区盒 8 段属于早期辫状河沉积向晚期曲流河沉积逐渐转化的沉积背景,其主要沉积微相包括河道滞留沉积、心滩、边滩、决口扇、天然堤、河漫砂及泛滥泥。 受基准面升降与沉积物供应的共同作用,该区河流相砂体演化呈阶段性变化,大致经历了辫状河繁盛发育期、辫-曲共存转化发育期及曲流河繁盛发育期 3 个阶段,其中辫状河繁盛发育期的心滩砂体与辫-曲共存转化发育期的心滩及边滩砂体是主力含气储层。 研究区优质储集砂体的发育受沉积微相展布与基准面旋回的控制。     

PdY8.5Ru0.19合金膜氚老化效应的TEM研究

PdY8.5Ru0.19合金是用于氢同位素分离的膜材料,但涉氚操作后,衰变3He会滞留在合金膜中并形成氦泡,影响其宏观性能.为了解PdY5.5Ru0.19合金膜贮氚老化后,3He在合金膜中的存在形式及分布状态.利用TEM观察分析了贮氚老化45和290 d的PdY8.5Ru0.19合金膜.实验结果表明:在老化45 d的样品中,观察到分布均匀,直径约1 nm的氦泡,同时存在高密度的位错及位错环.在老化290 d的样品中,氦泡直径略微增加,达1.2～1.4nm,且分布均匀,但位错及位错环密度降低.同时,在合金膜中也观察到因氦泡存在而产生的微裂纹与褶皱,这有可能是导致合金膜贮氚后力学性能下降的原因.     

石墨镶嵌Co纳米晶的形成及其特性

用直流碳弧法在阳极石墨棒中加入金属Ｃｏ产生石墨镶嵌Ｃｏ纳米晶,研究在复合石墨棒中加入不同的Ｃｏ含量对石墨镶嵌Ｃｏ纳米晶的形貌、结构特性及晶粒尺寸分布的影响,探讨石墨镶嵌Ｃｏ纳米晶的形成原因及碳弧法中氦气压力和Ｃｏ含量对掺Ｃｏ阳极石墨棒所产生的碳灰的Ｃ６０／７０产率的影响。结果表明,复合阳极棒中的Ｃｏ含量决定了石墨镶嵌Ｃｏ纳米晶的数量和晶凿直径分布,碳弧法中的Ｈｅ气压力仍是影响掺Ｃｏ阳极棒所产生的碳     

Soliton-Like Spin State in the A-Like Phase of 3He in Anisotropic Aerogel

We have found a new stable spin state in the A-like phase of superfluid ³He confined to intrinsically anisotropic aerogel. The state can be formed by radiofrequency excitation applied while cooling through the superfluid transition temperature and its NMR properties are different from the standard A-like phase obtained in the limit of very small excitation. It is possible that this new state is formed by textural domain walls pinned by aerogel.      

Formation of nanostructures in Ti2AlC induced by high-temperature helium irradiation

The effects of helium (He) irradiation on Ti₂AlC at different temperatures were studied in this work. He irradiation at room temperature (RT) induced severe lattice distortion and caused serious cracks in the samples. During He irradiation, Ti-Al bonds were easily broken and He atoms tended to accumulate at basal planes forming microcracks after irradiations at RT and 430 °C. Stacking faults and nanotwins were formed after He irradiation at all temperatures. Three kinds of nanostructures were formed after He irradiation: 1) face-centered cubic (fcc) nanotwins generated by outward diffusion of Al, accumulation of C interstitials and detwinning of Ti₂C slabs; 2) fcc nanograins induced by the formation of fcc structure and its subsequent amorphization by irradiation; 3) Ti₂AlC nanotwins induced by recrystallization from fcc nanotwins at 750 °C. All the results indicate that Ti₂AlC is highly resistant to He radiation and has excellent damage recovery at high temperatures.     

鄂尔多斯宁县-正宁地区上古生界盒8段天然气成藏特征及主控因素

鄂尔多斯宁县-正宁地区上古生界石盒子组盒₈段天然气展示了良好的勘探前景,但有效储层单层厚度薄、横向变化快,其天然气成藏特征和富集规律尚不清楚,严重制约了该区天然气勘探开发。为此,通过对研究区气藏生、储、盖、圈、运等成藏条件综合分析,总结其成藏特征和富集规律,筛选了气层敏感的测井曲线,结合储层岩性和物性特征,建立了研究区盒₈段气藏有效储层划分标准,在此基础上运用三维地震资料开展有效储层预测。结果表明:二叠系煤系烃源岩广覆式分布,处于高—过成熟阶段,为天然气成藏提供了良好的气源条件;盒₈段辫状河三角洲前缘分支河道砂岩近南北向条带状大规模展布,岩性主要为岩屑石英砂岩,次为石英砂岩,形成了天然气藏的有效储集砂体;盒₈段优势储层与下伏有效烃源岩形成“下生上储 ”型近源成藏组合,形成大面积展布的致密砂岩岩性气藏。近源有利砂体优先成藏,气藏分布及含气丰度受有效砂体展布、储层物性及通源断层控制。通过该研究落实了区内盒₈段有效储层分布,为该区域天然气下步勘探目标优选提供了依据。     

Ti-T靶中~3He测量

一、引言轻元素在材料中的含量及分布情况,是应用物理、应用技术等领域感兴趣的问题。目前,国外正在用各种核技术对此进行测量和研究。通常使用的Ti-T靶,因T的β衰变(T_(1/2)为12.33a),靶内~3He的含量将随制成靶的时间不同而变化。本文试图通过对不同时间制备的Ti-T靶中~3He的测量,探索测量和分析~3He的某种途径。     

Neutron Diffraction Study of He Solidified in a Mesoporous Glass

He embedded in a porous glass has been studied by neutron diffraction. Along the isochoric path studied, about 30% of the pore filling solidify in the bcc structure at 1.7 K and remain in this state down to 60 mK, the minimum temperature of the experiment. The other part of the pore filling is either liquid or an amorphous solid. The behaviour is discussed in terms of a thermodynamic model.     

不同温度下~3He 计数管热中子灵敏度测定

采用 DOT3.5(R,Z)迁移程序和 CITATION(R,Z)扩散程序,对含有~(252)Cf 中子源的石墨棱柱装置进行了通量分布计算,并用 DOT3.5(R,Z)程序计算了计数管对热通量的扰动因子。测量了~3He 和 BF_3(WL-6307)计数管的热中子灵敏度;测量结果表明,在20—150℃内,~3He 计数管热中子灵敏度几乎是不变的。