新型无机-有机杂化微孔晶体Cd3(BDC)0.5(BTC)2(DMF)(H2O)·3DMF·H3O·H2O的合成与结构

传统分子筛是以硅氧四面体和铝氧四面体为骨架的微孔晶体材料. 近年来, 以无机-有机结构单元为骨架组成的微孔晶体材料已引起人们的广泛关注[1～19]. 该类材料是由金属离子(或金属氧簇)与有机配体(大多数是芳香多酸和多碱)构成的建筑单元通过共价键或者分子间作用力构成的. 无机-有机杂化晶体材料有多种结构类型, 如1-D, 2-D, 3-D和笼状结构等.     

A Weakly Nonlinear Model for Kelvin-Helmholtz Instability in Incompressible Fluids

A weakly nonlinear model is proposed for the Kelvin-Helmholtz instability in two-dimensional incompressible fluids by expanding the perturbation velocity potential to third order. The third-order harmonic generation effects of single-mode perturbation are analyzed, as well as the nonlinear correction to the exponential growth of the fundamental modulation. The weakly nonlinear results are supported by numerical simulations. Density and resonance effects exist in the development of mode coupling.     

混合驱动中直驱激光焦斑尺寸对点火性能的影响

研究针对混驱点火模型,保持直驱激光能量不变,针对1 200,1 400和1 500μm直驱光焦斑尺寸,采用数值模拟,研究其对点火性能的影响。研究表明：直驱光焦斑尺寸是影响混驱点火性能的敏感因素。1 500μm焦斑尺寸可实现近一维点火。1 400μm焦斑尺寸放能接近一维放能的40%。1 200μm焦斑尺寸点火失败,仅仅处于燃烧等离子体状态。分析表明,1 200μm焦斑尺寸条件下点火失败的原因是：其产生的局部强光强和高驱动不对称性,会导致燃料熵增加及燃料面密度扰动增加。燃料熵的增加将会降低燃料压缩性,不利于创造高温高压点火条件,形成的燃烧波较弱。燃料面密度扰动增加会导致燃烧后壳层不稳定性剧烈增长。推断在小焦斑尺寸条件下,弱燃烧波及高燃料面密度扰动增长,会导致高密度尖钉难以被有效点燃,无法形成升温与燃烧的正反馈。同时,燃料区域内界面不稳定性发展产生的尖钉结构将降低热斑温度,产生的气泡结构将引起热斑体积迅速变大,导致热斑快速降温乃至点火失败。     

Numerical Simulation of Anisotropic Preheating Ablative Rayleigh-Taylor Instability

The linear growth rate of the anisotropic preheating ablative Rayleigh-Taylor instability （ARTI） is studied by numerical simulations. The preheating model κ （T）=κSH [1＋f（T）] is applied, where f（T） is the preheating function interpreting the preheating tongue effect in the cold plasma ahead of the ablative front. An arbitrary coefficient D is introduced in the energy equation to study the influence of transverse thermal conductivity on the growth of the ARTI. We find that enhancing diffusion in a plane transverse to the mean longitudinal flow can strongly reduce the growth of the instability. Numerical simulations exhibit a significant stabilization of the ablation front by improving the transverse thermal conduction. Our results are in general agreement with the theory analysis and numerical simulations by Masse [Phys. Rev. Lett. 98 （2007） 245001].     

链状Silicalite-1分子筛的合成

在传统的合成体系中, 加入聚电解质聚二烯丙基二甲基胺盐酸盐(PDDA)自组装合成链状的Silicalite-1分子筛材料, 考察了PDDA的加入对产物的影响, 并对其进行了XRD和SEM表征.     

二维可压缩流体Kelvin-Helmholtz不稳定性

利用高精度数值格式,研究了二维可压缩流体中的Kelvin-Helmholtz不稳定性,主要研究了可压缩性对Kelvin-Helmholtz稳定性增长率的影响.模拟定量的给出低Mach和高Mach数两种情况下,初始静压和对流Mach数以及Kelvin-Helmholtz不稳定性线性增长率的关系.模拟结果和自由剪切层以及混合层的实验结果以及理论分析一致.模拟表明,对流Mach数是描述流体可压缩性的合适参数,对流Mach数越小流体越不可压,Kelvin-Helmholtz不稳定性的线性增长率随对流Mach数的增加而减小. 关键词： Kelvin-Helmholtz不稳定性 可压缩流体 Mach数 超音速流体     

Multimode Coupling Theory for Kelvin-Helmholtz Instability in Incompressible Fluid

A weakly nonlinear model is proposed for multimode Kelvin-Helmholtz instability. The second-order mode coupling formula for Kelvin-Helmholtz instability in two-dimensional incompressible fluid is presented by expanding the perturbation velocity potential to second order. It is found that there is an important resonance in the course of the sum frequency mode coupling but the difference frequency mode coupling does not have. This resonance makes the sum frequency mode coupling process relatively complex. The sum frequency mode coupling is strongly dependent on time especially when the density of the two fluids is adjacent and the difference frequency mode coupling is not.     

经典瑞利-泰勒不稳定性界面变形演化的改进型薄层模型

激光惯性约束聚变(ICF)内爆靶丸通常采用多壳层组合结构设计,各壳层界面的流体力学不稳定性影响内爆加速和聚变点火,是ICF十分关心的问题.本文建立了描述任意Atwood数、任意初始界面分布Rayleigh-Taylor(RT)不稳定性界面变形及非线性演化的薄层模型.通过分析薄层中流体微团的受力,得到了运动微分方程组,并在二维情况进行数值求解.在线性阶段,薄层模型描述的界面演变规律与模拟结果符合很好;在非线性阶段,薄层模型可以描述至"蘑菇"形结构,与数值模拟的结果很接近.目前薄层的RT不稳定性非线性解析理论研究仅限于弱非线性阶段,本工作发展的薄层解析理论能很好地研究薄层非线性"气泡-尖钉"发展过程.     

Jet-Like Long Spike in Nonlinear Evolution of Ablative Rayleigh–Taylor Instability

We report the formation of jet-like long spike in the nonlinear evolution of the ablative Rayleigh-Taylor instability （ARTI） experiments by numerical simulations. A preheating model k（T） = KSH[1＋f（T）], where KSH is the Spitzer Harm （SH） electron conductivity and f（T） interprets the preheating tongue effect in the cold plasma ahead of the ablative front [Phys. Rev. E 65 （2002） 57401], is introduced in simulations. The simulation results of the nonlinear evolution of the ARTI are in general agreement with the experiment results. It is found that two factors, i.e., the suppressing of ablative Kelvin Helmholtz instability （AKHI） and the heat flow cone in the spike tips, contribute to the formation of jet-like long spike in the nonlinear evolution of the ARTI.     

基于1,1’-二苯乙炔-3,3’,5,5’-四羧酸微孔铜配位聚合物的合成和气体吸附性质

本文报道了配合物[Cu2(EBTC)(H2O)2]·8H2O·DMF.DMSO(1,EBTC=1,1′-二苯乙炔-3,3′,5,5′-四羧酸根;DMF=N,N-二甲基甲酰胺;DMSO=二甲基亚砜)的合成、晶体结构和吸附性质。1拥有内径为0.85 nm和0.85 nm×2.15 nm的两种孔洞,分别被6个和12个四羧酸根桥联的[Cu2(CO2)4]螺旋桨式结构围绕,并被EBTC连接成三维超分子结构,该结构拥有可容纳溶剂分子的一维孔道。1为(3,4)-连接的fof(sqc1575)拓扑结构,具有非常大的孔体积,其值高达单位晶胞体积的72.8%。去除溶剂分子后的1a表现出永久孔性,其Langmuir表面积为2844 m2·g-1,BET表面积为1 852 m2·g-1。它对H2、CO2、CH4和C2H2具有可观的气体吸附量和相对较高的吸附焓。特别是,在迄今所有已报道的孔性金属-有机材料中,1a在273 K、1.0×105Pa下,表现出最高的乙炔吸附量(252 cm3·g-1)和很高的吸附焓(吸附量为1 mmol·g-1时的吸附焓为34.5 kJ·mol-1)。