介观尺度多孔材料的电子显微学结构解析

孔径在介观尺度的多孔材料由于其规整的孔道结构、大比表面积、特殊的空间限域效应使其在吸附、分离、催化、传感、载药、能源等领域都具有广阔的应用前景. 深入解析材料的结构特征不仅是理解其物理化学性能和应用的关键, 也是研究材料的形成机理及新材料制备的重要反馈和支持. 电子显微学以电子为探针, 通过电子衍射和高分辨像对材料结构展开探索, 可以研究更小尺寸晶体的结构, 揭示局部结构信息如缺陷及共生等, 对介观尺度多孔材料的结构解析至关重要. 对近年来通过电子显微学方法解析的介观尺度多孔材料工作进行了综述, 主要针对有序介孔材料以及有序大孔材料展开, 归纳了不同结构类型的介观尺度多孔材料所适用的电子晶体学方法, 在此基础上提出电子显微学在介观尺度孔材料结构解析上的优势、不足和未来发展的方向, 以及将电子显微学用于其它材料结构解析的可行性.     

研究沸石结构的低剂量高分辨电子显微学方法

介绍了一种研究沸石结构的低剂量高分辨电子显微学方法,该方法可以有效降低电子束对沸石样品的辐照损伤,获得的高分辨像的分辨率优于0．18nm。提出了降低电子辐照损伤的措施,阐述了低剂量高分辨成像技术的技术要点。     

多羟基化合物法制备五次孪晶银纳米线的生长机理

运用多羟基化合物方法, 在添加表面活性剂聚乙烯吡咯烷酮(PVP) K30的溶液中合成了多次孪晶银纳米颗粒和纳米线. 运用透射电子显微术(TEM)和光吸收谱, 对不同的摩尔比n(PVP):n(AgNO3)和不同的搅拌条件下制备的纳米线进行了对比研究. 结果表明, 这种方法的制备过程中不仅存在由五个{111}面包裹成的锥形生长, 而且还同时存在垂直于生长方向的{110}层状生长, 并且两者之间还存在着竞争; 另外对纳米线的弯折处进行的高分辨电子显微学研究表明, 纳米线制备过程中遭受的塑性变形在纳米线中产生了大量的层错和位错; 纳米线折断产生的新鲜断口容易成为新的晶粒形核位置.     

含少量共聚组分聚乙烯熔体拉伸薄膜的形态结构

利用透射电子显微学(TEM)和示差扫描量热学(DSC)等方法研究了含少量丁烯-1组分(摩尔分数为0.64%)的聚乙烯共聚物(PE100)熔体拉伸高取向薄膜的形态结构. 结果表明, 在PE100熔体拉伸薄膜中, 除存在高取向片晶结构外, 还含有大量的纤维晶, 纤维晶平行于拉伸方向, 穿过几个片晶区, 平均直径约为12 nm. 模拟实验结果表明, 纤维晶的生成源于聚乙烯共聚物中的超高分子量组分, 但不同于传统意义上的伸直链纤维晶, 其形态特征应为晶桥结构. 由此提出了晶桥结构纤维晶模型, 该模型不但有助于深入理解和认识聚合物取向结晶机理, 同时也为该材料的高性能化提供了理论依据.     

HDPE,LLDPE或LDPE高取向薄膜微结构的电子显微学研究

木工作用透射电子显微术及电子衍射技术研究3种PE(HDPE,LLDPE或LDPE)均聚物高取向薄膜的微结构。定量测定了它们的结晶尺寸。通过倾斜样品电子显微学研究确定了不同种PE纤维结构的对称性。     

纳米碳酸钙/庚二酸复合成核剂对热致相分离法制备聚丙烯微孔膜的影响

以大豆油/邻苯二甲酸二丁酯(DBP)为混合稀释剂,采用热致相分离法(TIPS)制备聚丙烯(PP)微孔膜.研究了纳米碳酸钙成核剂、纳米碳酸钙/庚二酸复合成核剂对PP/大豆油/DBP(30/42/28,质量比)混合体系中PP结晶、熔融性能和PP微孔膜微观结构的影响.结果表明,单一纳米碳酸钙成核剂加入量为PP的0%~4%(质量百分率)时,PP/DBP/大豆油体系中PP熔融曲线上对应的峰值温度(Tpm)降到150.7~151.3℃,而纯PP的熔融峰值温度为165℃;DSC实验结果还显示加入1%~4%纳米碳酸钙和0.5%庚二酸后,导致PP的熔融曲线上出现了熔融双峰,说明纳米碳酸钙/庚二酸复合成核剂与单一成核剂相比有明显地促进β晶生成的作用,宽角X射线衍射(WAXD)实验进一步证实了β晶的存在.单一纳米碳酸钙成核剂对PP微孔膜的球晶结构和微观孔结构影响不大;加入纳米碳酸钙/庚二酸复合成核剂明显影响PP微孔膜的球晶结构和微观孔结构,其中0.5%庚二酸和1%纳米碳酸钙组成的复合成核剂制得的PP微孔膜的球晶结构明显,微孔膜孔径小且分布均匀;进一步增加纳米碳酸钙用量,PP微孔膜生成了许多细小的边界模糊的不规则结晶,微孔膜孔径不规则且尺寸较大,这与此时PP形成β晶结构有关.     

Armchair型石墨纳米带的电子结构和输运性质

利用第一性原理的电子结构和输运性质计算方法, 研究了扶手椅(armchair)型单层石墨纳米带(具有锯齿边缘)的电子结构和输运性质及其边缘空位缺陷效应. 研究发现, 完整边缘的扶手椅型石墨纳米带是典型的金属性纳米带, 边缘空位缺陷的存在对扶手椅型纳米带能带结构有一定的影响,但并不彻底改变其金属性特征.     

通过熔体自由基反应调控聚丙烯体系的链结构和相结构

熔融反应加工是聚合物改性和制备聚合物纳米复合材料的重要途径之一.在此过程中,多数加成聚合物由于受到热、剪切或引发剂作用,通常可原位形成大分子自由基反应中间体.我们系统地研究了如何利用这类大分子自由基调控聚合物分子链的拓扑结构和聚合物纳米复合体系的相结构与界面.然而,某些聚合物大分子自由基,如聚丙烯(PP),受其分子链化学结构决定,在熔融反应条件下非常易于发生降解.研究发现,将可控自由基聚合中调控自由基反应活性的方法应用在熔融反应过程中可以显著抑制PP的降解,促进主反应的发生,在制备长链支化聚合物、调控聚合物纳米复合材料的相结构方面发挥了重要作用.本文介绍了本研究组近几年来通过熔体自由基反应调控PP体系的链结构和相结构的相关研究工作,如实现PP的长链支化,制备高熔体强度PP;在制备PP/C60 、PP/碳纳米管(CNTs)纳米复合材料过程中,利用熔体界面区域所发生的自由基反应,提高了纳米粒子与PP的界面相互作用,改善了纳米粒子在PP中的分散状态等.     

聚丙烯-聚乙烯嵌段共聚物和相应共混物的热分析

用DSC研究了预期为聚丙烯-聚乙烯两嵌段共聚物(PP-PE)和相应共混物(PP+PE)在热学性能上的差异。经用不同分子量的PP和PE及其共混物进行试验后发现,由于PP和PE在结晶时出现过冷的难易不同。在共混物降温热分析曲线上,当降温速率较快时仅出现一个放热峰,而降温速率较慢时出现PP和PE各自的结晶放热峰,从而解释了文献中的不同结果。并发现共混物的PP和PE熔融、结晶温度均较组分相同的嵌段共聚物的相应温度为高;嵌段共聚物中PP和PE的△H_f值均低于均聚物的△H_f值,而PE的值降低尤甚。我们认为这与嵌段间的共价键限制嵌段活动和结晶过程有关,从而确认DSC热分析可以作为识别是否为嵌段共聚物的一种方法. 本工作的结果表明,所研究的PP-PE试样具有嵌段结构。     

iPP/HDPE/EPDM三元共混体系的组分分布、相容性和结晶行为

用DSC、~(13)C-NMR、SEM和WAXD等方法研究了IPP/HDPE/EPDM三元共混体系的组分分布、相容性和结晶行为。实验结果表明,EPDM与PE组分的相容性优于与PP组分的相容性,多数EPDM分子链段能够分布在PE组分中;EPDM含量为15％时,共混物相容性最好,SEM照片呈现晶体微区的互连或网络状结构;随EPDM含量增加,总结晶度X_c减小,其中PE组分结晶度X_(cE)有较大幅度地降低,PP组分结晶度X_(cp)基本没有变化,这可以根据EPDM和PE、PP之间相容性的差异以及PE、PP两组分在冷却过程中不同的结晶行为来解释。     

Vacuum Ultraviolet Photolysis of Polyethylene,Polypropylene, and Polystyrene

Using infrared reflection absorption spectroscopy (IRRAS), quartz crystal microbalance (QMB) measurements, and X-ray photoelectron spectroscopy (XPS) in combination with chemical derivatization techniques the VUV photolysis of polyethylene (PE), polypropylene (PP), and polystyrene (PS) was investigated. A mass balance obtained from the quantification of the data was used to suggest reaction path ways. Although PE and PP behave similar, the mass loss is about 8 times higher in the case of PP. These differences originate from the higher disproportionation to recombination ratio for the branched polymer. Both polymers form double bonds and at extended treatment times they tend to crosslink. PS is rather stable due to the possibility of the energy dissipation by fluorescence.     

Vacuum Ultraviolet Photolysis of Polyethylene,Polypropylene, and Polystyrene

Using infrared reflection absorption spectroscopy (IRRAS), quartz crystal microbalance (QMB) measurements, and X-ray photoelectron spectroscopy (XPS) in combination with chemical derivatization techniques the VUV photolysis of polyethylene (PE), polypropylene (PP), and polystyrene (PS) was investigated. A mass balance obtained from the quantification of the data was used to suggest reaction path ways. Although PE and PP behave similar, the mass loss is about 8 times higher in the case of PP. These differences originate from the higher disproportionation to recombination ratio for the branched polymer. Both polymers form double bonds and at extended treatment times they tend to crosslink. PS is rather stable due to the possibility of the energy dissipation by fluorescence.     

Polymer decoration study in chain folding behavior of solution-grown poly(ethylene oxide) crystals

The polymer decoration method based on the vaporization and condensation-crystallization of polyethylene (PE) upon the fold surface of polymer crystals has been widely used to study the chain folding behavior of the crystals. When this method was utilized to study solution-grown high molecular weight poly (ethylene oxide) (PEO) lamellar crystals, the highly anisotropic, low molecular weight fragment PE decorated become oriented parallel to the fold direction and form rods, which can be observed by transmission electron microscopy (TEM) and electron diffraction (ED). The growth sectors were clearly observed. From the ED patterns the {200} planes of the orthorhombic low molecular weight PE rod crystals can be observed, and the c-axis of these crystals is aligned parallel to the {120} growth planes of the PEO crystals. The decoration results indicate that the major fold orientation of high molecular weight PEO single crystals grown from dilute solution is along the {120} planes. © 1995 John Wiley & Sons, Inc.     

Effect of carbon nanotubes content on crystallization kinetics and morphology of polypropylene

Thermoplastic nanocomposites were prepared in a laboratory mixer using polypropylene (PP) and different amounts of single-walled carbon nanotubes (SWNT) in the range 0.25–2 wt%. The effect of SWNT content on the thermal and mechanical properties and also morphology of the PP/SWNT nanocomposites were studied. The results obtained from nonisothermal crystallization of PP and the nanocomposites, which were carried out using the differential scanning calorimetry technique, showed that not only the overall rate of crystallization of PP increased when SWNT was added to the polymer but also the rate of nucleation was higher and the crystallite size distribution was more uniform for the nanocomposites than for PP. From the optical microscopy studies, it was found that the PP spherulites decreased in size when SWNT was introduced into the polymer and also the mature spherical shaped crystals of PP changed in part to the immature kidney- or bean-shaped crystal forms in the nanocomposites. In addition, the crystallization kinetics was also studied by using isothermal spherulitic growth rate, and the values of nucleation constant, K_g, and end surface free energy, σ_e, were calculated for PP and the nanocomposites according to Lauritzen–Hoffman theory. The reductions of these two parameters were in agreement with the fact that the rate of crystallization of PP in nanocomposites was higher than that of the pristine polymer.     

Morphology and Crystal Structure of Wholly Aromatic All-Para Polyamide-Hydrazide Polymers

The morphology of some amide-hydrazide polymers of the type useful for high-modulus X-500 class fibers has been characterized by transmission electron microscopy of thin films crystallized from dilute solution. Selected area electron diffraction was used to characterize the crystallinity and crystal structure of the thin films and precipitated polymer. The films were cast from concentrated solutions and crystallized by heating the films. The results of these studies revealed several unique features relative to the crystal structure of the all-para polymers. Thin films of the crystallized polymer showed a distinctive crystalline texture—the molecular chains were found to be preferentially oriented parallel to the film plane and randomly oriented about an axis normal to the film plane. Electron diffraction measurements showed equatorial reflection maxima at tilt angles of = 30, ±48, and =59 when the films were tilted on an axis parallel to the film plane. From these results a tentative crystal unit cell and theoretical crystal density were determined: a = 8.5 [Agrave], b = 4.9 Å, c (chain axis) = 29.6 Å, p (density) =1.51 g/cc. The value a/b = 1.735, which is very near 3¹/², implies essentially hexagonal packing of the chains. Crystallization from dilute solution revealed lamellar structures resembling “single crystals” in the electron microscope similar to those observed in other crystalline polymers. However, in contrast to these other polymers, these “crystals” are not likely to contain folded chains because of the very rigid nature of the all-para poiyamide-hydrazide.     

Monte Carlo simulations of single crystals from polymer solutions

A novel "anisotropic aggregation" model is proposed to simulate nucleation and growth of polymer single crystals as functions of temperature and polymer concentration in dilute solutions. Prefolded chains in a dilute solution are assumed to aggregate at a seed nucleus with an anisotropic interaction by a reversible adsorption/desorption mechanism, with temperature, concentration, and seed size being the control variables. The Monte Carlo results of this model resolve the long-standing dilemma regarding the kinetic and thermal roughenings, by producing a rough-flat-rough transition in the crystal morphology with increasing temperature. It is found that the crystal growth rate varies nonlinearly with temperature and concentration without any marked transitions among any regimes of polymer crystallization kinetics. The induction time increases with decreasing the seed nucleus size, increasing temperature, or decreasing concentration. The apparent critical nucleus size is found to increase exponentially with increasing temperature or decreasing concentration, leading to a critical nucleus diagram composed in the temperature-concentration plane with three regions of different nucleation barriers: no growth, nucleation and growth, and spontaneous growth. Melting temperatures as functions of the crystal size, heating rate, and concentration are also reported. The present model, falling in the same category of small molecular crystallization with anisotropic interactions, captures most of the phenomenology of polymer crystallization in dilute solutions.     

Mixed crystal infrared study of chain folding in crystalline polyethylene

Infrared spectroscopic studies have been made of mixed crystals of linear polyethylene and perdeuteropolyethylene. On the basis of normal vibration analyses by Tasumi and Krimm it had been shown that the study of crystal splittings of internal chain modes in such mixed crystals could provide information on the geometry of chain folding. The present results, which include a study of n-paraffin (C₃₆) mixed crystals, confirm these predictions. They show that (110) folding predominates in dilute solution grown crystals, and that this is transformed to (200) folding in melt-crystallized polymer. Folding with adjacent re-entry is favored, a random re-entry model being clearly eliminated.     

Nano-structured,semicrystalline polymer foams

Semicrystalline polymers gelled from thermally quenched semidilute solutions can, in some cases, be supercritically dried to produce nano-structured foams of exceedingly high specific surface area. This article investigates the nano-morphology of these semicrystalline foams. The common morphological feature that these systems display in small-angle scattering can be described by uncorrelated lamellar platelets. The morphological details, which can be obtained using microscopy and small-angle scattering, indicate that these low-density systems occupy a morphological niche between polymeric crystallites from dilute solutions, and spherulitic crystals derived from concentrated solutions and melts. Because these crystalline morphologies occur in concentration ranges between dilute and concentrated, they may offer simple insight into the mechanisms available for distortion of ideal, dilute-solution-derived crystallites as polymer concentration is increased. Several mechanisms for the observed distortions are proposed. © 1996 John Wiley & Sons, Inc.     

Solution annealing of poly(TMPS) crystal mats

Poly(tetramethyl-p-silphenylene siloxane) crystal mats initially prepared from benzene/methanol (2:1 v/v), when annealed in small amounts of solvent undergo considerable thickening in the chain direction. When the crystals are annealed above their formation temperature, their physical properties change rapidly at first before reaching an asymptotic limit commensurate with annealing time and type of solvent. Changes in melting temperature, heat of fusion, small-angle x-ray spacing, and wide-angle x-ray scattering patterns have been monitored for three solvents of varying solvent power, ranging from very good to extremely poor. Upon solution annealing, the original crystals mats equilibrate to more stable dimensions compatible with their environment. The activation energy of crystal thickening in contact with a liquid is estimated to be about an order of magnitude lower than that deduced from dry annealing data. It appears that the crystal surface and the crystalline core of the crystals comprising the mats must participate in the measured severalfold increase in long period noted after annealing. The lower surface (or interfacial) energy of the liquid annealed mats compared to isothermally melt-crystallized polymer of similar molecular weight has a direct bearing on the polymer morphology and crystallinity.     

Epitaxial crystallization of homopolymers on single crystals of alkali halides

Epitaxial deposition of homopolymers from solution [polyethylene, isotactic polystyrene, poly-3,3-bischloromethyloxacyclobutane (Penton) and polypropylene] was found on the (001) faces of cleaved alkali halide single crystals. Electron and optical microscopy studies have shown that the polymer usually grew from small, rodlike crystallites which were oriented in (110) directions of the halide crystal. Large oriented, four-leaved, “rose” structures also were observed for polyethylene. Electron diffraction studies indicate that the polymer chain axes for polyethylene, isotactic polystyrene, and Penton generally lie parallel to the (001) faces of the halide crystal and are also oriented in the 〈110〉 directions of the crystal face. Investigations on the effect of various halide substrates upon the epitaxial crystallization habit of polyethylene inferes that lattice matching does not play the major role in orientation. Two possible explanations are offered for this epitaxial behavior.