玉兰花粉个体发育及绒毡层动态

苏联植物学家A．L．塔赫他间在<有花植物（木兰植物）分类大纲>(Ta-khtaian，1980)中认为广义的木兰目是最原始的和最古老的类群，由它产生被子植物所有其它主要分枝。根据这个观点，作者试图以木兰科玉兰(Magnol iadenudata Desr.)，花粉个体发育为主题，探讨它们的原始性状、特点及其在系统发育上的地位。 下面就其花粉个体发育顺序，扼要概括如下： 1．小孢子母细胞、减数分裂到四分体时期：细胞器发生重组，质体和线粒体发生脱分化与再分他的循环。在此期间，细胞中还有大量胞质小泡，高尔基体小泡参与胼胝质壁物质的形成，其他小泡与脂体物质的沉积有关。晚二分体时期，原外壁物质开始沉积，胞质小泡可能涉及原外壁的形成和未来萌发孔的位置。 2．游离小孢子时期：细胞器变得丰富而活跃，特别是粗糙内质网大量出现，它们与脂体的形成和运输有关。此时，外壁外层已形成，外壁内层和内壁开始发育。 3．两细胞花粉时期;质体出现极性分布，生殖细胞中不含质体。生殖细胞随着位置的推移，其形状和壁的结构、性质也发生变化，生殖细胞由凸透镜形变成球形以至梭形。同时，生殖细胞壁最初含纤维素和胼胝质物质，以后壁物质逐渐消失，当生殖细胞变为梭形时，在生殖细胞壁的双层膜间又出现亲锇物质沉积。有趣的是，在生殖细胞星球形时，营养细胞中的脂体紧挨并围绕生殖细胞，形成一层明显的脂体冠。 玉兰成熟花粉为远极单槽，营养细胞中造粉体里园球形，内部充满大量均匀小淀粉颗粒，生殖细胞形状特殊，在有丝分裂前两极具明显的细胞质延伸和突起。从花粉个体发育着，玉兰花粉壁带有若干裸子植物性状和原始特征。最重要的特点表现在：①外壁内层具片层状结构;②I柱：状层虽具稀疏小柱，但在孢壁分沁过程中，”在小柱之问还有大小不同的孢粉素颗粒;③在萌发孔处，外壁外层往往扩张、外折，形似穗花杉和香榧的残余气囊。玉兰花粉的内壁特殊，由内壁-l、内壁-2和内壁-3等三层形状和质地不同的结构组成。值得注意的是百合科的麝香百合内壁也呈明显不同的三层结构。 玉兰绒毡层为多层细胞，属分泌型。绒毡层细胞中细胞器很丰富，减数分裂期问达到高峰。细胞核明显地被质体和线粒体所包围。粗糙内质网常与膳体连在一起。四分体时期，原乌氏体排出，孢粉素在其上沉积。推测原乌氏体和孢粉素前体物质的形成与粗糙内质网活动和膳体形成有关，乌氏体有单个存在，也有以聚乌氏体或复合乌氏体形式出现。周绒毡层膜在二分体时期即开始形成，最初呈间断的薄膜小片，以后连续发育成膜。周绒毡层膜位于靠药壁细胞的绒毡层细胞四周及中层绒毡层细胞外切向面，而靠药室腔的绒毡层细胞则未见此膜。 总之，玉兰的生殖细胞特殊，附带脂体冠;后期呈梭形，两极具明显的胞质延伸和突起，不含质体。孢壁结构具明显原始性状，在某种意义上，一方面类似裸子植物，另一方面又有百合科的特点。绒毡层结构也有一些值得深入探讨的问题。

白皮松（Pinus bungeana）和青杄（Picea wilsonii）花粉脱壁技术建立及细胞学研究

花粉是种子植物受精过程中雄性生殖细胞的载体，在有性生殖过程中起着非常重要的作用。花粉与柱头、花柱、子房等都有相互作用，起识别作用的是细胞壁蛋白，而花粉粒的壁有明显的两层：内壁和外壁。裸子植物花粉与被子植物相比具有萌发时间长、生长缓慢、授粉－受精时间长等特点。花粉的内壁与外壁在花粉萌发和生长过程中的功能仍然缺乏研究，但是迄今为止现有的分子生物学技术在获得裸子植物花粉壁突变体方面并没有发挥作用。本研究以裸子植物白皮松(Pinus bungeana)和青杄（Picea wilsonii）花粉为材料建立裸子植物花粉脱壁的体系，包 括脱外壁花粉和花粉原生质体的制备，即将花粉的两层壁逐层剥离，并在此基础上进行了细胞学研究。 本文首先建立了裸子植物脱外壁花粉的分离技术。实验表明低浓度的酶组合短暂酶解后，辅以机械研磨，可以释放出大量的脱外壁花粉。其中在这两种裸子植物中的处理稍有不同，白皮松的脱外壁花粉在含12％蔗糖，0.5%纤维素酶和0.3%离析酶的溶液，pH 5.8 ，孵育半小时，辅以一定力度机械研磨的方法获得，而青杄脱外壁花粉的条件是0.8%纤维素酶和0.5%离析酶、12％蔗糖的溶液，其它条件类似。 其次我们成功建立了一种快速、有效、可重复的分离白皮松和青杄花粉原生质体的系统，分离频率可高达70%。对白皮松而言，最好的分离条件是2% 纤维素酶、1.5%离析酶、15%蔗糖、pH 5.8，黑暗、24℃条件下轻微振荡、酶解6 小时。3％纤维素酶和2％离析酶组合比较适宜青杄花粉原生质体的分离，同时需要较低浓度的蔗糖溶液（12％）。青杄花粉原生质体要远大于白皮松花粉原生质体，前者直径为80µm，后者为40µm。强烈的FDA 荧光显示很好的活性。在制备的过程中，酶的浓度、酶的配比、酶解时间、渗透压调节剂、起始材料对分离率都有影响。 运用免疫荧光标记技术显示，脱外壁花粉的表面存在纤维素、果胶质、阿拉伯半乳聚糖蛋白（AGPs）和凝集素结合位点，其中纤维素在整个表面都有分布，但在萌发孔附近的荧光最强;白皮松脱外壁花粉表面有胼胝质的存在，主要位于靠近气囊的部位，而青杄脱外壁花粉表面未能检测到胼胝质;酸性果胶质在白皮松脱外壁花粉靠近萌发孔处的荧光稍弱于其它部位，而在青杄脱外壁花粉的表面近极端的荧光要强于远极端;白皮松脱外壁花粉表面有酯化果胶的沉积，而青杄脱外壁花粉表面缺失酯化果胶;白皮松和青杄两种植物脱外壁花粉表面均有阿拉伯半乳糖的分布，而白皮松脱外壁花粉的荧光要远强于青杄;白皮松和青杄脱外壁花粉表面有伴刀豆凝集素（Conconavalin agglutinin, Con A ）和大豆凝集素（soybean agglutinin, SBA ）结合位点的分布，而缺失麦胚凝集素（wheat germ agglutinin, WGA）结合位点。另外，傅立叶红外光谱(FTIR) 分析结果也同样支持上述结论。

Microstructure and Evolution of Mechanically-Induced Ultrafine Grain in Surface Layer of Al-Alloy Subjected to USSP

Experiments were conducted to investigate the ultrafine-grained (UFG) microstructures in the surface layer of an aluminum alloy 7075 heavily worked by ultrasonic shot peening. Conventional and high-resolution electron microscopy was performed at various depths of the deformed layer. Results showed that UFG structures were introdued into the surface layer of 62 μm thick. With increasing strain, the various microstructural features, e.g., the dislocation emission source, elongated microbands, dislocation cells, dislocation cell blocks, equiaxed submicro-, and nano-crystal grains etc., were successively produced. The grain subdivision into the subgrains was found to be the main mechanism responsible for grain refinement. The simultaneous evolution of high boundary misorientations was ascribed to the subgrain boundary rotation for accommodating further strains. Formed microstructures were highly nonequilibratory.  2002 Acta Materialia Inc. Published by Elsevier Science Ltd. All rights reserved.

Partial-Dislocation-Mediated Processes in Nanocrystalline Ni with Nonequilibrium Grain Boundaries

The partial-dislocation-mediated processes have so far eluded high-resolution transmission electron microscopy studies in nanocrystalline nc Ni with nonequilibrium grain boundaries. It is revealed that the nc Ni deformed largely by twinning instead of extended partials. The underlying mechanisms including dissociated dislocations, high residual stresses, and stress concentrations near stacking faults are demonstrated and discussed.

Influence of grain boundary on melting

The temperature behaviour of an Al bicrystal with surfaces consisting of (110) and (111) crystals is simulated using molecular dynamics. The result shows that the (110) crystal losses its crystalline order at 820K, whereas the disorder does not propagate through the (111) crystal at this temperature. Instead, some disordered atoms are recrystallized into the (111) crystal and the initial grain boundary changes into a stable order-disorder interface. Thus, it was discovered that at a temperature near its melting point, the (111) crystal grew and obstructed the propagation of disorder. Such an obstruction is helpful for understanding melting.

Grain Refinement at the Nanoscale Via Mechanical Twinning and Dislocation Interaction in a Nickel-Based Alloy

A nanostructured surface layer was formed on an Inconel 600 plate by subjecting it to surface mechanical attrition treatment at room temperature. Transmission electron microscopy and high-resolution transmission electron microscopy of the treated surface layer were carried out to reveal the underlying grain refinement mechanism. Experimental observations showed that the strain-induced nanocrystallization in the current sample occurred via formation of mechanical microtwins and subsequent interaction of the microtwins with dislocations in the surface layer. The development of high-density dislocation arrays inside the twin-matrix lamellae provides precursors for grain boundaries that subdivide the nanometer-thick lamellae into equiaxed, nanometer-sized grains with random orientations.

Localized Solid-State Amorphization at Grain Boundaries in a Nanocrystalline Al Solid Solution Subjected to Surface Mechanical Attrition

Using high-resolution electron microscopy, localized solid-state amorphization (SSA) was observed in a nanocrystalline (NC) Al solid solution (weight per cent 4.2 Cu, 0.3 Mn, the rest being Al) subjected to a surface mechanical attrition treatment. It was found that the deformation-induced SSA may occur at the grain boundary (GB) where either the high density dislocations or dislocation complexes are present. It is suggested that lattice instability due to elastic distortion within the dislocation core region plays a significant role in the initiation of the localized SSA at defective sites. Meanwhile, the GB of severely deformed NC grains exhibits a continuously varying atomic structure in such a way that while most of the GB is ordered but reveals corrugated configurations, localized amorphization may occur along the same GB.

The Influence of Grain Size and Temperature on the mechanical Deformation of Nanocrystalline Materials: Molecular Dynamics Simulation

Nanocrystalline (nc) materials are characterized by a typical grain size of 1-100nm. The uniaxial tensile deformation of computer-generated nc samples, with several average grain sizes ranging from 5.38 to 1.79nm, is simulated by using molecular dynamics with the Finnis-Sinclair potential. The influence of grain size and temperature on the mechanical deformation is studied in this paper. The simulated nc samples show a reverse Hall-Petch effect. Grain boundary sliding and motion, as well as grain rotation are mainly responsible for the plastic deformation. At low temperatures, partial dislocation activities play a minor role during the deformation. This role begins to occur at the strain of 5%, and is progressively remarkable with increasing average grain size. However, at elevated temperatures no dislocation activity is detected, and the diffusion of grain boundaries may come into play.

Strain-Induced Grain Refinement of Cobalt During Surface Mechanical Attrition Treatment

The microstructural evolution during surface mechanical attrition treatment of cobalt (a mixture of hexagonal close packed (hep) and face-centered cubic (fcc) phases) was investigated. In order to reveal the mechanism of grain refinement and strain accommodation. The microstructure was systematically characterized by both cross-sectional and planar-view transmission electron microscopy. In the hcp phase, the process of grain refinement. Accompanied by an increase in strain imposed in the surface layer. Involved: (1) the onset of 110 111 deformation twinning, (2) the operation of (1 120) 110 1 0} prismatic and (1 120) (000 1) basal slip, leading to the formation of low-angle dislocation boundaries, and (3) the successive subdivision of grains to a finer and finer scale. Ressulting in the formation of highly misoriented nanocrystalline grains. Moreover. The formation of nanocrystalliies at the grain boundary and triple junction was also observed to occur concurrently with straining. By contrast. The fec phase accommodated strain in a sequence as follows: (1) slip of dislocations by forming intersecting planar arrays of dislocations, (2) {1 1 1} deformation twinning, and (3) the gamma(fcc) --> epsilon(hcp) martensitic phase transformation. The mechanism of grain refinement was interpreted in terms of the structural subdivision of grains together with dynamic recrystallization occurring in the hep phase and the gamma --> E: martensitic transformation in the fcc phase as well.

Dislocations And Twins In Nanocrystalline Ni After Severe Plastic Deformation: The Effects Of Grain Size

Deformation microstructures have been investigated in nanocrystalline (nc) Ni with grain sizes in the 50-100 nm range. It was found that deformation twinning started to occur in grains of similar to 90 nm, and its propensity increased with decreasing grain size. In most of the nc grains dislocations were observed as well, in the form of individual dislocations and dipoles. It is concluded that dislocation-mediated plasticity dominates for grain sizes in the upper half, i.e. 50-100 nm, of the nanocrystalline regime. (C) 2007 Published by Elsevier B.V.

Inverse Grain-Size Effect On Twinning In Nanocrystalline Ni

A long-standing controversy exists between molecular dynamics simulations and experiments on the twinning propensity of nanocrystalline (NC) face-centered-cubic metals. For example, three-dimensional molecular dynamics simulations rarely observed twins in NC Ni, whereas experiments readily observed them. Here this discrepancy is resolved by experimental observation of an inverse grain-size effect on twinning. Specifically, decreasing the grain size first promotes twinning in NC Ni and then hinders twinning due to the inverse grain-size effect. Interestingly, no inverse grain-size effect exists on stacking fault formation. These observations are explained by generalized planar fault energies and grain-size effect on partial emissions.

Grain Boundary Effects On Plastic Deformation And Fracture Mechanisms In Cu Nanowires: Molecular Dynamics Simulations

Metallic nanowires have many attractive properties such as ultra-high yield strength and large tensile elongation. However, recent experiments show that metallic nanowires often contain grain boundaries, which are expected to significantly affect mechanical properties. By using molecular dynamics simulations, here, we demonstrate that polycrystalline Cu nanowires exhibit tensile deformation behavior distinctly different from their single-crystal counterparts. A significantly lowered yield strength was observed as a result of dislocation emission from grain boundaries rather than from free surfaces, despite of the very high surface to volume ratio. Necking starts from the grain boundary followed by fracture, resulting in reduced tensile ductility. The high stresses found in the grain boundary region clearly play a dominant role in controlling both inelastic deformation and fracture processes in nanoscale objects. These findings have implications for designing stronger and more ductile structures and devices on nanoscale.

Small scale, grain size and substrate effects in nano-indentation experiment of film-substrate systems

The mechanical properties of film-substrate systems have been investigated through nano-indentation experiments in our former paper (Chen, S.H., Liu, L., Wang, T.C., 2005. Investigation of the mechanical properties of thin films by nano-indentation, considering the effects of thickness and different coating-substrate combinations. Surf. Coat. Technol., 191, 25-32), in which Al-Glass with three different film thicknesses are adopted and it is found that the relation between the hardness H and normalized indentation depth h/t, where t denotes the film thickness, exhibits three different regimes: (i) the hardness decreases obviously with increasing indentation depth; (ii) then, the hardness keeps an almost constant value in the range of 0.1-0.7 of the normalized indentation depth h/t; (iii) after that, the hardness increases with increasing indentation depth. In this paper, the indentation image is further investigated and finite element method is used to analyze the nano-indentation phenomena with both classical plasticity and strain gradient plasticity theories. Not only the case with an ideal sharp indenter tip but also that with a round one is considered in both theories. Finally, we find that the classical plasticity theory can not predict the experimental results, even considering the indenter tip curvature. However, the strain gradient plasticity theory can describe the experimental data very well not only at a shallow indentation depth but also at a deep depth. Strain gradient and substrate effects are proved to coexist in film-substrate nano-indentation experiments. (c) 2006 Elsevier Ltd. All rights reserved.