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。

Nifedipine调节白皮松(Pinus bungeana)花粉管蛋白质表达及其对细胞壁构建的影响

花粉管是种子植物受精过程中的雄性生殖单位的载体，由于其生长依赖于胞内Ca2+梯度，并具有典型的顶端极性生长的特点，因而成为近年来研究植物细胞相互识别、胞内和胞外信号传导理想的模式系统。裸子植物花粉与被子植物相比具有萌发时间长、生长缓慢等特点。Ca2+在裸子植物花粉萌发和花粉管生长中的作用机制目前尚不明确。本研究以裸子植物白皮松(Pinus bungeana)的花粉为材料，运用不同浓度钙通道抑制剂Nifedipine（Nif）处理，对其花粉萌发和花粉管生长进行了细胞学研究和蛋白质组学分析，以探讨Ca2+对白皮松花粉生长的调控机制，为进一步揭示裸子植物花粉萌发和花粉管生长机理提供参考。 本论文首先研究了钙通道抑制剂Nif和Ca2+螯合剂EGTA对白皮松花粉萌发和花粉管生长的影响。结果表明，用Nif处理花粉后，花粉萌发和花粉管生长均受到明显抑制。经Ca2+荧光探针Fluo-3AM标记，对Nif处理后Ca2+在花粉管中的分布模式进行了观察，发现Ca2+在正常生长的花粉管中呈梯度分布，并在其顶端的荧光最强。与对照相比，处理后的花粉管荧光强度明显减弱，且顶端Ca2+梯度消失。通过EGTA漂洗后的花粉粒，在正常培养基上萌发率较高，但其生长速率受到抑制。由此说明了细胞壁钙库对花粉管生长的抑制效应显著高于对花粉萌发的影响，是花粉管生长的限速因子。同时外加钙调素还可逆转EGTA对其花粉萌发和花粉管生长的抑制。上述结果表明，白皮松花粉萌发及花粉管生长需要外源Ca2+的内流，以及胞内形成的Ca2+浓度梯度。 用FM4-64探针标记结果发现，正常花粉管中的胞吞作用主要发生在顶端和亚顶端区域，胞吞的小泡也集中分布在这两个区域。经Nif处理后，既不影响花粉管的胞吞过程，同时胞吞发生的位置也与对照相似，只是胞吞的小泡分散于整个花粉管中。电子显微镜观察表明，各种细胞器在白皮松正常生长的花粉管中分布与被子植物存在较大差异，例如前者无明显地分区现象，不具胼胝质塞。白皮松花粉管顶端和亚顶端的壁旁体与质膜融合现象频繁发生。花粉管经Nif处理后，线粒体出现不同程度的解体和液泡化，内质网液泡化和核糖体脱落，液泡大量聚集在花粉管顶端，壁旁体与膜融合现象减少，以及花粉管壁明显变薄等。此外，通过微丝特异性探针鬼笔环肽标记结果表明，正常生长花粉管的微丝呈长轴向排列， Nif处理后微丝断裂，其断裂程度与处理浓度有关。由此可见，外源Ca2+对花粉管的胞吞无明显抑制或促进作用，但对胞吞小泡重回收可能有影响。当胞内Ca2+梯度消失后，则明显抑制了微丝骨架的聚合，进而使胞吐作用减缓，高尔基体分泌小泡聚集，多种细胞器液泡化，引起花粉管顶端膨大，细胞壁变薄，继而抑制花粉管的正常生长。 运用免疫荧光标记技术显示，正常生长的花粉管壁含有纤维素、胼胝质、果胶质和阿拉伯半乳聚糖蛋白（AGPs），其中纤维素和胼胝质在细胞壁上呈均匀分布，而酸性果胶质只存在花粉管两侧壁上，酯化果胶分布于花粉管顶端。经过Nif处理后，胼胝质和酸性果胶质均在花粉管顶端累积，而AGPs和纤维素的分布却无明显变化。另外，傅里叶红外光谱分析结果也同样支持上述结论。通过花粉管壁蛋白的SDS-PAGE分析表明，Nif对细胞壁蛋白的合成也有较大的影响。 在花粉管的钙通道受到抑制后，应用蛋白质组学技术分析其蛋白质的表达图谱，通过双向电泳已分离出约1000个蛋白质斑点，经软件分析发现，除其中50个蛋白斑点外，大部分蛋白质的表达量均未发生变化。上述50个发生变化的蛋白斑点酶切后，再经过ESI－MS/MS鉴定和质谱数据库的搜索，共鉴定出28个蛋白，其中12个为上调蛋白，16个下调蛋白，根据其主要功能分为与代谢、细胞扩展、翻译后修饰以及信号相关的蛋白。经过Nif处理后，花粉管中碳水化合物代谢能力下降，ATP的产生受到抑制，参与细胞壁多糖合成及小泡运输的蛋白，如valosin containing protein（VCP）、reversibly glycolsylated polypeptide(RGP)、UDP-glucose dehydrogenase (UDPGDH)和α-tubulin表达下调。另外，通过上述方法还鉴定出与丝氨酸/苏氨酸激酶保守结构域同源的受体蛋白激酶等。 综上所述，白皮松花粉管钙通道受到抑制后，通过影响花粉管蛋白的表达，抑制微丝微管骨架的组装，致使胞吐速度变慢，花粉管壁酸性果胶质、胼胝质等多糖分布的变化及总多糖含量的减少，最终抑制了花粉管的正常生长。

Transport of anti-sperm monoclonal IGA and IGC into murine male and female genital tracts from blood - Effect of sex hormones

Ab levels in the genital tract may be important in fertility and in preventing sexually transmitted diseases, In this study, I-125-labeled polymer or monomer mAb IgA (C4pIgA or C4mIgA) and IgC2b (C4IgC) to murine lactate dehydrogenase C4 and a polymer mAb IgA (npIgA) not cross-reacting with mouse sperm were intravenously injected into BALB/c mice, and the relative distribution of these Abs was determined. Polymer IgA was transported much more efficiently into the genital tract, trachea, and duodenum of both sexes than C4IgG and C4 mIgA (p < 0.01), The transport of polymer IgA (C4pIgA and npIgA) into the male genital tract greatly increased following orchiectomy (p < 0.01); this change was not affected by testosterone, suggesting that the unknown regulatory factor(s) from the testis may suppress polymer IgA transport, However, the transport of polymer IgA into female genital tissues was significantly decreased by ovariectomy (p < 0.01); this decline can be rectified by P-estradiol but not progesterone treatment, suggesting that estradiol may stimulate polymer IgA transport, Furthermore, the transport of C4IgG into tissues of the Fallopian tubes and the uterus was significantly decreased by treatment with progesterone (p < 0.01). Together, these findings indicate that serum polymer IgA can be transported selectively into the genital tracts of both sexes, that this transport is strongly under the control of gonads, and that transport of Ige into the Fallopian tubes and uterus is downregulated by progesterone.

Influence of ion energy and deposition temperature on the surface morphology of carbon films deposited by ion beams

Carbon films were deposited by mass-selected ion beam technique with ion energies 50-200eV at a substrate temperature from room temperature to 80 degreesC,. For the energies used, smooth diamond-like carbon films were deposited at room temperature. When the substrate temperature was 600 degreesC,rough graphitic films were produced. But highly oriented carbon tubes were observed when the energies were larger than 140eV at 800 degreesC. They were perpendicular to the surface and parallel to each other. preferred orientation of graphite basic plane was observed by high-resolution electron microscopy. Shallow ion implantation and stress are responsible for this orientation.

Chaotic behavior of pulsating heat pipes

Chaotic behavior of closed loop pulsating heat pipes (PHPs) was studied. The PHPs were fabricated by capillary tubes with outer and inner diameters of 2.0 and 1.20 mm. FC-72 and deionized water were used as the working fluids. Experiments cover the following data ranges: number of turns of 4, 6, and 9, inclination angles from 5 degrees (near horizontal) to 90, (vertical), charge ratios from 50% to 80%, heating powers from 7.5 to 60.0 W. The nonlinear analysis is based on the recorded time series of temperatures on the evaporation, adiabatic, and condensation sections. The present study confirms that PHPs are deterministic chaotic systems. Autocorrelation functions (ACF) are decreased versus time, indicating prediction ability of the system is finite. Three typical attractor patterns are identified. Hurst exponents are very high, i.e., from 0.85 to 0.95, indicating very strong persistent properties of PHPs. Curves of correlation integral versus radius of hypersphere indicate two linear sections for water PHPs, corresponding to both high frequency, low amplitude, and low frequency, large amplitude oscillations. At small inclination angles near horizontal, correlation dimensions are not uniform at different turns of PHPs. The non-uniformity of correlation dimensions is significantly improved with increases in inclination angles. Effect of inclination angles on the chaotic parameters is complex for FC-72 PHPs, but it is certain that correlation dimensions and Kolmogorov entropies are increased with increases in inclination angles. The optimal charge ratios are about 60-70%, at which correlation dimensions and Kolmogorov entropies are high. The higher the heating power, the larger the correlation dimensions and Kolmogorov entropies are. For most runs, large correlation dimensions and Kolmogorov entropies correspond to small thermal resistances, i.e., better thermal performance, except for FC-72 PHPs at small inclination angles of theta < 15 degrees.

Uniform mems chip temperatures in the nucleate boiling heat transfer region by selecting suitable, medium boiling number range

The not only lower but also uniform MEMS chip temperatures can he reached by selecting suitable boiling number range that ensures the nucleate boiling heat transfer. In this article, boiling heat transfer experiments in 10 silicon triangular microchannels with the hydraulic diameter of 55.4 mu m were performed using acetone as the working fluid, having the inlet liquid temperatures of 24-40 degrees C, mass fluxes of 96-360 kg/m(2)s, heat fluxes of 140-420 kW/m(2), and exit vapor mass qualities of 0.28-0.70. The above data range correspond to the boiling number from 1.574 x 10(-3) to 3.219 x 10(-3) and ensure the perfect nucleate boiling heat transfer region, providing a very uniform chip temperature distribution in both streamline and transverse directions. The boiling heat transfer coefficients determined by the infrared radiator image system were found to he dependent on the heat Axes only, not dependent on the mass Axes and the vapor mass qualities covering the above data range. The high-speed flow visualization shows that the periodic flow patterns take place inside the microchannel in the time scale of milliseconds, consisting of liquid refilling stage, bubble nucleation, growth and coalescence stage, and transient liquid film evaporation stage in a full cycle. The paired or triplet bubble nucleation sites can occur in the microchannel corners anywhere along the flow direction, accounting for the nucleate boiling heat transfer mode. The periodic boiling process is similar to a series of bubble nucleation, growth, and departure followed by the liquid refilling in a single cavity for the pool boiling situation. The chip temperature difference across the whole two-phase area is found to he small in a couple of degrees, providing a better thermal management scheme for the high heat flux electronic components. Chen's [11 widely accepted correlation for macrochannels and Bao et al.'s [21 correlation obtained in a copper capillary tube with the inside diameter of 1.95 mm using R11 and HCFC123 as working fluids can predict the present experimental data with accepted accuracy. Other correlations fail to predict the correct heat transfer coefficient trends. New heat transfer correlations are also recommended.

Are the available boiling heat transfer coefficients suitable for silicon microchannel heat sinks?

The typical MEMS fabrication of micro evaporators ensures the perfect smooth wall surface that is lack of nucleation sites, significantly decreasing the heat transfer coefficients compared with miniature evaporators fabricated using copper or stainless steel. In the present paper, we performed the boiling heat transfer experiment in silicon triangular microchannel heat sink over a wide parameter range for 102 runs. Acetone was used as the working fluid. The measured boiling heat transfer coefficients versus the local vapor mass qualities are compared with the classical Chen’s correlation and other correlations for macro and miniature capillary tubes. It is found that most of these correlations significantly over-predict the measured heat transfer coefficients. New correlations are given. There are many reasons for such deviations. The major reason is coming from the perfect smooth silicon surface that lowers the heat transfer performances. New theory is recommended for the silicon microchannel heat sink that should be different from metallic capillary tubes.