The Interaction Between Shock Waves and Solid Spheres Arrays in a Shock Tube

When a shock wave interacts with a group of solid spheres, non-linear aerodynamic behaviors come into effect. The complicated wave reflections such as the Mach reflection occur in. the wave propagation process. The wave interactions with vortices behind each sphere's wake cause fluctuation in the pressure profiles of shock waves. This paper reports an experimental study for the aerodynamic processes involved in the interaction between shock waves and solid spheres. A schlieren photography was applied to visualize the various shock waves passing through solid spheres. Pressure measurements were performed along different downstream positions. The experiments were conducted in both rectangular and circular shock tubes. The data with respect to the effect of the sphere array, size, interval distance, incident Mach number, etc., on the shock wave attenuation were obtained.

Experimental Investigation On The Slip Between Oil And Water In Horizontal Pipes

This work is devoted to study of the slip phenomenon between phases in water-oil two-phase flow in horizontal pipes. The emphasis is placed on the effects of input fluids flow rates, pipe diameter and viscosities of oil phase on the slip. Experiments were conducted to measure the holdup in two horizontal pipes with 0.05 m diameter and 0.025 m diameter, respectively, using two different viscosities of white oil and tap water as liquid phases. Results showed that the ratios of in situ oil to water velocity at the pipe of small diameter are higher than those at the pipe of big diameter when having same input flow rates. At low input water flow rate, there is a large deviation on the holdup between two flow systems with different oil viscosities and the deviation becomes gradually smaller with further increased input water flow rate. (C) 2008 Elsevier Inc. All rights reserved.

Study of drag reduction by gas injection for power-law fluid flow in horizontal stratified and slug flow regimes

In this work, the drag reduction by gas injection for power-law fluid flow in stratified and slug flow regimes has been studied. Experimentswere conducted to measure the pressure gradient within air/CMC solutions in a horizontal Plexiglas pipe that had a diameter of 50mm and a length of 30 m. The drag reduction ratio in stratified flow regime was predicted using the two-fluid model. The results showed that the drag reduction should occur over the large range of the liquid holdup when the flow behaviour index remained at the low value. Furthermore, for turbulent gas-laminar liquid stratified flow, the drag reduction by gas injection for Newtonian fluid was more effective than that for shear-shinning fluid, when the dimensionless liquid height remained in the area of high value. The pressure gradient model for a gas/Newtonian liquid slug flow was extended to liquids possessing the Ostwald–de Waele power law model. The proposed model was validated against 340 experimental data point over a wide range of operating conditions, fluid characteristics and pipe diameters. The dimensionless pressure drop predicted was well inside the 20% deviation region for most of the experimental data. These results substantiated the general validity of the model presented for gas/non-Newtonian two-phase slug flows.

Studies on two-phase co-current air/non-Newtonian shear-thinning fluid flows in inclined smooth pipes

In this work. co-current flow characteristics of air/non-Newtonian liquid systems in inclined smooth pipes are studied experimentally and theoretically using transparent tubes of 20, 40 and 60 turn in diameter. Each tube includes two 10 m lone pipe branches connected by a U-bend that is capable of being inclined to any angle, from a completely horizontal to a fully vertical position. The flow rate of each phase is varied over a wide range. The studied flow phenomena are bubbly, plug flow, slug flow, churn flow and annular flow. These are observed and recorded by a high flow. stratified flow. -speed camera over a wide range of operating conditions. The effects of the liquid phase properties, the inclination angle and the pipe diameter on two-phase flow characteristics are systematically studied. The Heywood-Charles model for horizontal flow was modified to accommodate stratified flow in inclined pipes, taking into account the average void fraction and pressure drop of the mixture flow of a gas/non-Newtonian liquid. The pressure drop gradient model of Taitel and Barnea for a gas/Newtonian liquid slug flow was extended to include liquids possessing shear-thinning flow behaviour in inclined pipes. The comparison of the predicted values with the experimental data shows that the models presented here provide a reasonable estimate of the average void fraction and the corresponding pressure drop for the mixture flow of a gas/ non-Newtonian liquid. (C) 2007 Elsevier Ltd. All rights reserved.

Notch sensitivity of circular rings subjected to impact loading

'Notch-sensitive regions' have been observed during a series of experimental investigations into the dynamic plastic behaviour and failure of thin-walled metallic radially notched circular rings with are-shaped supports subjected to concentrated impact loads. The experimental results show that the exterior notches at some regions have no effect on the deformation of the rings, but do have effect at the remaining regions. The notch-sensitive region is theoretically determined by using the equivalent structures technique; fairly good agreement has been reached between the simple theory and the experimental results. Both dimensional and theoretical analyses prove that whether a plastic hinge formed or not at the notched section does not depend on the mean radius of the ring and the input kinetic energy. It depends on the weak coefficient of the notched section and the angle of the support. Generally speaking, there are mainly three failure modes for a notched circular ring with are-shaped support under impact loading: Mode I, large inelastic deformation when the notch is outside the sensitive region, in this case the ring deforms as a normal one; Mode II, large inelastic deformation only at some part of the ring and tearing occurred at the notched sections; Mode III, large inelastic deformation and total rupture occurred at the notched sections. It is believed that the present study could assist the understanding of the dynamic behaviour and failure of other kinds of nonstraight components with macroscopic imperfections under impulsive loading.

Reflection of shock-wave in pur foam from rigid wall

Keller proposed that a building, a mechanical installation or a body wrapped bya layer of foam plastics may be an efficient means for protection from damage ofblast wave. However, the practical effect was beyond expectation. For example, agunner wearing the foam plastics-padded waistcoat was injured more seriously by theblast wave from a muzzle. Monti took the foam plastics as homogeneous two-phasemedium and analyzed it with the theory of dusty flow. The obtained results showthat the peak pressure behind the reflected shock wave from rigid wall with foamcoat exceeds obviously that without foam coat under the same condition. Gel'fand,Patz and Weaver made experimental observations by means of shock tubes and veri-

High-speed streams from coronal holes and the accelerating mechanism of the solar-wind

In this paper, the general Mach number equation is derived, and the influence of typical energy forms in the solar wind is analysed in detail. It shows that the accelerating process of the solar wind is influenced critically by the form of heating in the corona, and that the transonic mechanism is mainly the result of the adjustment of the variation of the crosssection of flowing tubes and the heat source term.The accelerating mechanism for both the high-speed stream from the coronal hole and the normal solar wind is similar. But, the temperature is low in the lower level of the coronal hole and more heat energy supply in the outside is required, hence the high speed of the solar wind; while the case with the ordinary coronal region is just the opposite, and the velocity of the solar wind is therefore lower. The accelerating process for various typical parameters is calculated, and it is found that the high-speed stream may reach 800 km/sec.

激波管双爆轰驱动段性能的数值模拟研究

采用频散可控的耗散格式(DCD),求解Euler方程和一种改进的二阶段化学反应模型,对氢氧反向-正向双爆轰驱动段激波管进行了数值模拟.计算结果表明:当辅驱动段与主驱动段初始压力比小于临界值时,Taylor波仍会出现,但波扇夹角较单一前向爆轰驱动段小,入射激波马赫数衰减率变小;当初始压力比等于临界值时,主驱动段中的Taylor波完全被消除,入射激波马赫数不再衰减.当初始压力比大于临界值时,在主驱动段中能产生过驱动爆轰波,不仅Taylor波被完全消除,而且驱动能力较单一前向爆轰驱动段强

水平分支管路中油水两相流动研究

该文研究了两种直径的直管油水两相流动对流型和相含率的影响和在不同管径的水平并行分支管路中的相含率变化规律。实验设备包括内径为50mm的水平主管道和内径为25mm的分支管路。得到了不同入口条件下实验管段的流型和相含率图。实验指出:管道的尺度变化对于流型的影响较小,但对于油水两相的相含率和速度滑移有显著的作用。当油水两相流在并行分支管路中同时流动时,随着入口处水的表观流速增大,并行主管的截面油含率与并行分支管的差距逐渐缩小。

Influence of Contact Angle and Tube Size on Capillary-Driven Flow Under Microgravity

The influence of contact angle and tube radius on the capillary-driven flow for circular cylindrical tubes is studied systematically by microgravity experiments using the drop tower. Experimental results show that the velocity of the capillary flow decreases monotonically with an increase in the contact angle. However, the time-evolution of the velocity of the capillary flow is different for different sized tubes. At the beginning of the microgravity period, the capillary flow in a thinner tube moves faster than that in a thicker tube, and then the latter overtakes the former. Therefore, there is an intersection between the curves of meniscus velocity vs microgravity time for two differently sized tubes. In addition, for two given sized tubes this intersection is delayed when the contact angle increases. The experimental results are analyzed theoretically and also supported by numerical computations.

Subwavelength imaging by a dielectric-tube photonic crystal

In contrast to previous two-dimensional coated photonic crystals, in this paper we propose a left-handed one that is made of dielectric tubes arranged in a close-packed hexagonal lattice. Without metallic cores, this structure is low-loss and convenient to fabricate. Negative refraction and its resulting focusing are investigated by dispersion characteristic analysis and numerical simulation of the field pattern. With proper modification at the interface, the image is improved. With better isotropy than that with noncircular rods, planoconcave lenses made by dielectric tubes focus a Gaussian beam exactly at R//n - 1/.

Subwavelength imaging with two symmetrical interfaces by dielectric-tube photonic crystals

As distinct from coated photonic crystals, in this paper we propose a novel one that is made of dielectric tubes arranged in a close-packet square lattice. Without metallic cores, this structure is low-loss and convenient to fabricate. A left-handed frequency region is found in the second band by dispersion characteristic analysis. Without inactive modes for the transverse electric mode, negative refraction and subwavelength imaging are demonstrated by the finite-difference time-domain simulations with two symmetrical interfaces, i.e. Gamma X and Gamma M.

Conductance calculation of a long tube with equilateral triangle cross section

Using the stratified gas flow model for calculating the conductance of long tubes with constant cross section, an analytical expression for calculating the conductance of along tube with equilateral triangle cross section has been derived. The formula given is applicable to the full pressure range. A minimum in the conductance in the intermediate flow state is shown. 2002 American vacuum Society.

甘蓝型油菜（Brassica napus L.）花粉和柱头的发育及其与自交不亲和性的关系

作者用扫描电镜、透射电镜和组织化学方法研究了甘蓝型油菜(Brassica napus L．)花粉和柱头的发育及相互作用,得到了如下结果： 一．甘蓝型油菜具有典型的同型孢子体自交不亲和性(Homomorphic and sporophytic self-incompatibility)。自花授粉后，部分花粉粘住在乳突细胞表面，随后萌发出花粉管，花粉管生长受阻于乳突细胞，花粉管表现出各种异常形态，缠绕卷曲(Coiled pattern),顶端膨大成基足状(pad-Like swelling),花粉管二叉分枝（dichotomous branching Pollen tubes），花粉管相互连接(connections of pollen tubes），有的花粉粒还形成两个花粉管。 二．不同时期的乳突细胞的扫描电镜观察表明： 开花前6—7天 乳突细胞壁内陷，柱头中央有一沟槽; 开花前4—5天 乳突细胞被有孔的块状物覆盖; 开花前2—3天 覆盖物消失，壁表面只剩下波状纹或小凹; 开花前l - 2天 乳突细胞充分吸水膨胀，呈指状，排列疏松，细胞壁上有一些小颗粒。此时的乳突细胞已发育成熟。 三.不亲和授粉时，花粉和乳突细胞均有强烈的胼胝质荧光。 四.乳突细胞的组织化学特点：缺乏淀粉积累，细胞壁和细胞质中有过氧化物酶活性。 五.乳突细胞的超微结构特点：细胞壁分为三层，蜡质层、角质层和纤维素层。粗面内质网成群分布在细胞壁附近，并以及泡形式向细胞壁分泌物质。缺乏质体，细胞核位于乳突细胞基部，细胞中央为大液泡占据。 六.花粉的超微结构发育特点：单核花粉已发育出内壁和外壁，外壁内层不明显。细胞核位于中央。细胞质浓厚，缺乏层膜结构而积累大量淀粉粒的质体存在于细胞质中。其他细胞器不发达。两细胞花粉时期，花粉壁接受乌氏体转运的孢粉素和含油体转运的脂类物质。生殖细胞没有壁，悬浮在营养细胞的细胞质中。细胞核大，细胞质稀薄，只有一些嵴不明显的线粒体。营养细胞的核显著，细胞质浓厚，线粒体发达，质体内部的淀粉消失，转变成嗜饿小体。内质网短而粗，遍布于细胞质中，高尔基体缺乏。 七.绒毡层积极参与了花粉外壁的建成。首先，它通过分泌作用把物质（可能是蛋白质）转移到单核花粉的腔隙中或在它后期滚解后，由分布在二细胞花粉间的粗面内质网合成蛋白质，转移到花粉壁内。其次，绒毡层细胞的质体层膜形成许多造油小体，至二胞花粉时，造油小体进入壁的柱状层，参与花粉鞘形成。第三，绒毡层细胞形成许多乌氏体，花粉发育后期，乌氏体与花粉外壁接触，将孢粉素转移到花粉外壁上。

白杄花粉管胞吞/胞吐动态及其与细胞壁构建的关系

在有花植物受精过程中，具有顶端极性生长特性的花粉管是雄性生殖单位的载体，同时也是研究细胞生长分子调控机理的理想体系。与被子植物相比，裸子植物花粉具有萌发时间长、花粉管生长缓慢等特点。对于裸子植物花粉萌发和花粉管生长的机理，目前人们尚不十分清楚。本文将以裸子植物白杄（Picea meyeri）花粉为材料，应用不同浓度的分泌系统干扰剂Brefeldin A处理，并通过细胞学和生理生化方法，其中包括普通光学显微镜、荧光显微镜、激光扫描共聚焦显微镜、显微红外光谱（FTIR）和透射电镜（TEM）等技术，对其花粉萌发和花粉管生长过程中胞吞胞吐的调控，以及与细胞壁建成的关系等进行较为系统的研究，旨在为进一步揭示裸子植物花粉管发育的调控机理提供参考。 首先比较观察了各种细胞器在白杄与被子植物花粉管中的分布差异。经FM4-64探针标记结果表明，在正常生长的白杄花粉管顶端存在分泌小泡积累的透明区，但与被子植物比较起来，此透明区在花粉管中所占比例较小，且不呈倒“V”字型。在透射电镜下观察发现，其花粉管顶端透明区内分泌小泡的分布密度远低于被子植物。另外，在白杄花粉管中，线粒体的分布一般靠近细胞壁的地方，高尔基体分布较为分散，而内质网的分布则不具方向性。 其次，研究了BFA对白杄花粉萌发和花粉管生长的影响，特别是对其花粉管生长过程中的胞吐/胞吞作用。通常在正常生长的白杄花粉管中，用FM4-64标记后发现，在其顶端形成与透明区对应的荧光亮区;超微结构显示，在花粉管顶端进行旺盛的胞吐作用，许多分泌小泡正与质膜融合，以及分布有大量显示高分泌活性的壁旁体（PB）等。而经过BFA处理后，花粉的萌发和花粉管的生长均受到严重抑制，花粉管出现了弯曲（波状生长）或顶端膨大等异常形态，同时还干扰了FM4-64在花粉管顶端的标记模式。另外，花粉管顶端分泌小泡数量减少，透明区内充满线粒体、高尔基体和空泡等一些大的细胞器，壁旁体也随之消失，其中高尔基体呈现解体或弯曲的异常形态，在其周围的分泌小泡数量大大减少，内质网出现膨胀和核糖体脱落等;同时胞吐活性标志性酶——酸性磷酸酶的活性也随之降低。通过对FM4-64的染料吸收实验表明，BFA对胞吞有明显的促进作用。由上可见，BFA对白杄花粉管生长过程中的胞吐和胞吞作用起了相反的影响， BFA正是通过扰乱花粉管生长过程中的分泌途径来抑制其花粉管的生长。 最后，检测了白杄花粉管分泌途径紊乱后，管壁物质合成的变化情况。通过FTIR光谱分析表明，BFA处理后花粉管壁化学组分发生了变化，例如蛋白质和多糖含量明显减少，而且与蛋白比较起来，多糖的含量下降更为明显，尤其是在顶端。蛋白和多糖含量的下降导致花粉管壁的组成结构不够致密。由SDS-PAGE的结果显示， BFA抑制后，花粉管壁中糖蛋白的含量下降了60%，同时很多壁蛋白条带在BFA处理后不表达或含量减少。通过对花粉管壁多糖成分的研究表明，BFA处理还导致纤维素含量下降，而胼胝质在花粉管顶端积累。用识别AGPs的LM6和识别酸性果胶的JIM5对花粉管进行标记，发现BFA处理后AGPs的环状分布消失，酸性果胶质在顶端的含量也明显减少，但在胞质内却形成一些小的分隔亮点（compartments）。 综上所述，导致裸子植物白杄花粉管生长缓慢的原因，可能与其顶端透明区较小、分泌小泡数量少等有关。另外，从白杄花粉管的细胞质状态和细胞器分布上看，虽然与被子植物相比差异较大，但在其正常生长中仍能进行旺盛地胞吐和胞吞过程。经BFA处理后引起花粉管内分泌系统的紊乱，致使管壁物质不能正常合成，从而导致花粉管的停滞生长。