Phase Transitions in Emulsions Formed by Aqueous Emulsifier and its Action on Improving Mobility in Oil Recovery

Transition from oil-in-water (O/W) emulsions to water-in-oil (W/O) emulsions and its action on enhanced oil recovery was investigated by viscosity, morphology, and simulated flooding experiments. This transition can be realized by increasing the volume ratio of oil to water or decreasing the emulsifier concentration. At a mass concentration of 0.3 wt%, the self-developed emulsifier FJ-1 mainly forms O/W emulsions at a volume ratio (oil to water) of 1:1. The emulsions behave as O/W emulsions with a low viscosity when the volume ratio of oil to water is below 2:1. Above 2:1, increasing volume ratio leads to the O/W emulsions transferring into W/O emulsions with high viscosity. For example, at a volume fraction of 4:1, the viscosity of W/O emulsions reaches 229.1 mPa · s, and separated water can hardly be detected. Transition from O/W emulsions to W/O emulsions with high viscosity can also be realized by decreasing the concentration of emulsifier to 0.05 wt% or lower at a volume ratio of 1:1. These may be the critical factors leading to transition from O/W emulsions to W/O emulsions at core conditions. Simulated flooding experiments show that emulsifier fluids can act as an in situ mobility improver and make an improvement of oil recovery even by 20.4%. The results indicate that the water-in-crude-oil emulsions possess great potential in enhancing oil recovery.     

Exact Three-Dimensional Relativistic Equation for qq Bound states

Starting with the QCD generating functional, a new derivation and a new form of the Dirac-Schriidinger (D-S) equation,catisfied by the equal-time Bethe-Salpeter amplitude of quark-antiquark bound states have been given. In this equation, the effective interaction kernel has a compact expression and can be directly calculated by means of the conventional QCD Feynman rules. F'urthermore, an equivalent reduction of the above equation to a Pauli-Schriidinger equation has also been achieved and a closed form of the effective interaction Hamiltonian appearing in the latter equation has been explicitly written out.     

衰减相移掩模及其编码制作方法研究

在霍普金斯理论的基础上,对方孔的传统掩模、衰减相移以及加入光学邻近效应校正的衰减相移掩模在硅片表面光强分布的计算表明,衰减相掩模有提高光刻分辨率的显著功能,提出一种制作衰减相移掩模的编码方法。理论计算表明,该编码方法能够达到预定的衰减参数。     

基于光时域反射技术与缠绕式光纤传感陈列的结构状态监测方法

提出了一种新颖的、利用多模光纤缠绕钢绳式的传感阵列网络,对智能材料与结构的受力、应变等状态参量进行了监测和估计,并采用了光时域反射技术实时处理并行分布式传感信号,给出了测试数据、识别结果.     

基于光时域反射技术与缠绕式光纤传感阵列的结构状态监测方法

提出了一种新颖的、利用多模光纤缠绕钢绳式的传感阵列网络, 对智能材料与结构的受力、应变等状态参量进行了监测和估计, 并采用了光时域反射技术实时处理并行分布式传感信号, 给出了测试数据、识别结果     

电化学STM技术在金属腐蚀科学中的应用及研究进展

本文介绍了电化学STM在金属腐蚀电化学研究领域的技术优势.其最大特点是可以在金属腐蚀环境中和原子/分子水平上,实时、原位、三维空间观察,并可以通过电位控制表面电极过程.综述了电化学STM在钝化膜结构、缓蚀剂的自组装膜、金属表面原子的活性溶解等揭示腐蚀缓蚀机理的研究领域中所起的重要作用以及最新研究进展.     

碳酸二甲酯法合成1,5-萘二氨基甲酸甲酯的反应机理

 应用红外光谱技术研究了在乙酸锌催化作用下1,5-萘二胺与碳酸二甲酯甲氧基羰基化反应机理. 结果表明,二水合乙酸锌只有失去两个结晶水变成无水乙酸锌后才能产生催化活性. 无水乙酸锌与1,5-萘二胺形成一个新的配位络合物,该配位络合物是一个适宜的亲核试剂,能与碳酸二甲酯进行亲核反应,生成1,5-萘二胺的甲氧基羰基化产物. 在无水乙酸锌与1,5-萘二胺形成配位络合物的过程中,无水乙酸锌的结构从双齿型转变成单齿型.     

柱前荧光衍生-高效液相色谱法测定尿和血清中的环境雌激素

建立了同时测定人尿和血清中环境雌激素双酚A、4-壬基酚、17α-乙炔基雌二醇及内源性雌激素雌三醇、17α-雌二醇和17β-雌二醇的对硝基苯甲酰氯柱前荧光衍生-高效液相色谱测定方法。尿样经酸水解、固相萃取柱浓缩、净化分离;血清样品经乙腈沉淀蛋白后,用乙醚萃取游离态雌激素,N2气流挥干、在无水条件下,雌激素与对硝基苯甲酰氯反应生成荧光产物,用高效液相色谱法定量。检出限为2．7—8．3μg／L;加标回收率尿样为78．0％-102．5％,血清样为72．6％-98．6％;方法精密度为1．29％-4．52％。应用本法对20份尿样和10份血清样进行了测定,结果满意。     

宽视场大相对孔径星敏感器光学系统设计

介绍了一种用于卫星姿态控制的星敏感器光学系统,该光学系统焦距为51 mm,相对孔径为1/1.1,视场角为21°×21°（圆视场2ω＝30°）,光谱范围为0.5～0.85 μm,采用了复杂化双高斯结构.与普通成像系统不同的是,该系统要求对不同光谱的恒星所采集到的点像能量中心是一致的,且星像点像的弥散圆须控制在一定的范围内.具有倍率色差小、轴上和轴外能量分布比较一致的特点.     

Numerical generation of hyperspherical harmonics for tetra-atomic systems

A numerical generation method of hyperspherical harmonics for tetra-atomic systems, in terms of row-orthonormal hyperspherical coordinates-a hyper-radius and eight angles-is presented. The nine-dimensional coordinate space is split into three three-dimensional spaces, the physical rotation, kinematic rotation, and kinematic invariant spaces. The eight-angle principal-axes-of-inertia hyperspherical harmonics are expanded in Wigner rotation matrices for the physical and kinematic rotation angles. The remaining two-angle harmonics defined in kinematic invariant space are expanded in a basis of trigonometric functions, and the diagonalization of the kinetic energy operator in this basis provides highly accurate harmonics. This trigonometric basis is chosen to provide a mathematically exact and finite expansion for the harmonics. Individually, each basis function does not satisfy appropriate boundary conditions at the poles of the kinetic energy operator; however, the numerically generated linear combination of these functions which constitutes the harmonic does. The size of this basis is minimized using the symmetries of the system, in particular, internal symmetries, involving different sets of coordinates in nine-dimensional space corresponding to the same physical configuration.