Cardinalities of poly(p-phenylene) graphs

Recurrence relation for the cardinalities of linear and cylindrical poly(p-phenylene) (PPP) compounds has been developed that requires the cardinalities of two of their immediate lower homologues. Such recurrence relation reduces into analytical expressions for the cardinalities under transfer matrix formalism. Ambient condition density and bulk modulus of linear PPPs are found to bear excellent linear correlation with the inverse of logarithm of their cardinalities. Topological bond orders obtained from the cardinalities of such PPPs have been found to have good linear correlations with the respective Hückel bond orders.     

Effect of the shell on the transport properties of poly(glycerol) and Poly(ethylene imine) nanoparticles

Dendritic core–shell architectures containing poly (glycerol) and poly (ethylene imine) cores and poly(lactide) shell (PG-PLA and PEI-PLA respectively) were synthesized. Analogous of these core–shell architectures containing the same cores but poly (L-lactide) shell (PG-PLLA and PEI-PLLA, respectively) were also synthesized. In this work PG and PEI were used as macroinitiator for ring opening polymerization of the lactid and L-lactide monomers. Different molar ratios of monomer to end functional groups of PG ([LA]/[OH]) and PEI ([LA]/[NHn] (n = 1 or 2)) were used to prepare the core–shell architectures with different shell thickness. These core–shell architectures were able to encapsulate and transport the small guest molecules. Their transport capacity (TC) depended on the type and thickness of the shells. TC of core–shell architectures containing PLLA shell was higher than that for their analogs containing PLA shell. The diameter of core–shell architectures was between 20–80 nm. The rate of release of guest molecules from chloroform solution of nanocarriers to water phase was investigated and it depended on the type of the core, shell and solvent.     

Phosphorescence of Poly(Methylphenyl)Silane Films

In the 5–100 K temperature range, the photoluminescence spectra of poly(methylphenyl)silane (PMPS) and polystyrene films doped with acetophenone, propiophenone, benzophenone, diphenyl, and naphthalene, as well as the thermostimulated luminescence spectra of neat PMPS films, have been investigated. It has been shown that the PMPS film phosphorescence spectrum consists of a structureless band with a maximum near 450 nm, and the literature structural phosphorescence spectrum of this polymer may belong to an uncontrolled impurity or a defect with chromophore groups of acetophenone.     

三螺旋DNA分子poly(dT)·poly(dA)·poly(dT)的构型和振动谱

我们计算了ｐｏｌｙ（ｄＴ）·ｐｏｌｙ（ｄＡ）·ｐｏｌｙ（ｄＴ）的Ｈｏｗａｒｄ模型的原子笛卡尔坐标，并利用晶格动力学方法对模型进行了简正分析。结果发现其０ Ｐ ０对称振动模式位于８０４ｃｍ－１，这和８１０ｃｍ－１附近没有拉曼和红外谱线的实验结果不符。在８００～１０００ｃｍ－１的范围内只有四个振动模式，明显少于拉曼和红外光谱在该范围内的谱线数目。所以我们认为Ｈｏｗａｒｄ模型需要进一步地完善和修正，ｐｏｌｙ（ｄＴ）·ｐｏｌｙ（ｄＡ）·ｐｏｌｙ（ｄＴ）必须具有三条不完全一致的脊骨     

Optical absorption and spectrophotometric studies on the optical constants and dielectric of poly (o-toluidine) (POT) films grown by spin coating deposition

In this work, a poly(o-toluidine) “POT” was synthesized by chemical oxidative polymerization method in aqueous media. High uniform and good adhesion thin films of POT have been successfully deposited by the spin coating technique. The films were characterized by X-ray diffraction (XRD) and Fourier transforms infrared (FTIR) spectroscopy. The XRD pattern of the POT shows the semi-crystalline nature of the films. FTIR studies show the information of functional groups in POT. The optical transmittance and reflectance of POT film was measured in the 200–2500 nm wavelength range. The absorption coefficient analysis shows that the optical band gaps of POT film are direct allowed transition band gaps with 1.2 and 2.6 eV. Other optical absorption parameters such as extinction molar coefficient, oscillator strength and electric dipole strength were also calculated. The dispersion parameters were determined and discussed based on the single oscillator model. According to the analysis of dispersion curves some important parameters such as dispersion energy (E_d), oscillator energy (E_o), high frequency dielectric constant ₍ε_∞) and lattice dielectric constant (ε_L) were also evaluated. Discussion of the obtained results and their comparison with the previous published data were also given. The obtained desirable results of POT thin film can be useful for the optoelectronic applications.     

分子量对氟苯-聚-α-甲基苯乙烯乳液固化速率的影响

为研究分子量对聚--甲基苯乙烯（PAMS）空心微球的乳液微封装制备过程中乳液固化速率的影响,实验采用分子量为300~800 kgmol-1的3种PAMS作为油相,测量在聚乙烯醇（PVA）和聚丙烯酸（PAA）两种外水相环境下,PAMS/氟苯（FB）乳液直径、油相浓度和FB扩散通量随固化时间的变化。结果表明,随PAMS分子量减小,PAMS油相浓度上升趋势变慢,FB扩散通量的峰值在分子量为300 kgmol-1时达到最小。因此,可通过降低PAMS分子量的方式来延长乳液的固化时间,从而降低FB的扩散速率,使乳液有足够时间调整形变有利于获得良好的微球球形度。     

Synthesis and spectral-luminescent properties of poly(N-isopropylacrylamide)

The spectral-luminescent characteristics of water and methanol solutions of polymers containing tetraphenylporphyrin substituents were investigated. The water-soluble polymer was obtained by the interaction of poly(N-isopropylamide) containing N-oxysuccinimide substituents with 5-(4-aminophenyl)-10,15,20-triphenylporphyrin. From the synthesized polymer its analog with Zn-porphyrin substituents was obtained. This phenomenon is attributed to the specific features of the conformational behavior of polymeric chains in water solutions. Water solutions of polymers experience a thermally reversible phase transition upon heating, which is accompanied by a considerable enhancement of light scattering. Translated from Zhurnal Prikladnoi Spektroskopii, Vol. 67, No. 4, pp. 483–487, July–August, 2000.     

Investigation of regeneration effect of blue luminescence in NaCl using variable delay optically stimulated luminescence (VD-OSL)

Optically stimulated luminescence (OSL) of pure analytical sodium chloride (NaCl) was studied. Performing series of CW-OSL (continuous wave OSL) readouts it was found that subsequent CW-OSL decay, after some delay, starts from significantly higher intensity level than the final intensity of the previous readout. To study this ‘regeneration effect’ a new type of measurements was implemented – the variable delay OSL (VD-OSL) method. The idea of VD-OSL is explained – it allows to study OSL kinetics at very long time scale. VD-OSL data confirm coexistence of two effects in NaCl – regeneration and fading of the OSL signal. After partial CW-OSL readout, regeneration predominates in the short time scale of the order of 10³ s. Then, fading becomes dominant. The same measurements were applied to commonly used Al₂O₃:C material as well. Nevertheless, the results do not show such behavior at the studied time scale. Theoretical arguments are presented that the regeneration mechanism cannot be explained on the basis of the simple trap model.     

石墨烯/聚乙撑二氧噻吩薄膜储能特性（英）

为了有效利用石墨烯和导电聚合物材料,光雕石墨烯/聚3,4-乙撑二氧噻吩(LSG/PEDOT)复合薄膜通过一种灵巧的光雕工艺制备出来。在此复合薄膜中,每种组分对薄膜的电化学性能提升都有独特的贡献。循环伏安、交流阻抗及恒流充放电测试用来检测薄膜的电化学性能。结果显示,在引入PEDOT纳米颗粒后,LSG/PEDOT复合薄膜显示出更好的能量存储能力。复合薄膜的比容量达到64.33 F/cm3,是光雕石墨烯比容量(3.89 F/cm3)的20倍,复合薄膜经过1000次循环后仍能保持初始容量的94.6%。复合薄膜电化学性能的提升主要是由于引入的PEDOT纳米颗粒既阻挡了石墨烯的层层堆叠,又增加了整个薄膜的比表面积。此种灵活的光雕工艺还可以用来大规模制备超级电容器电极。     

Light-induced metastable defects in a-Se90X10 (X = Sb,In and Ag) thin films

Thin films of chalcogenide glasses in a binary system of Se₉₀X₁₀ (X = Sb, In and Ag) have been prepared by the vacuum evaporation technique. Thermally stimulated current measurements have been made to find out the trap density in these materials. To study light-induced defects in these materials, white light of intensity 1200 lux is shown on the amorphous films in vacuum for different exposure times. It is observed that the density of traps increases with exposure time, indicating the appearance of light-induced metastable defects in these materials.     

A method for quantitative interpretation of fluorescence detection of poly(ethylene glycol)-mediated 1-palmitoyl-2-[[[2-[4-(phenyl-trans-1,3,5-hexatrienyl) phenyl]ethyl]oxyl]carbonyl]3-sn-phosphatidylcholine (DPHpPC) transfer and fusion between phospholipid vesicles in the dehydrated state

A method has been developed for calculating the expected fluorescence lifetime of the DPH _p PC probe distributed between different membrane environments. We show how this method can be used to distinguish between lipid transfer and fusion between large unilamellar vesicles occurring in the presence of poly(ethylene glycol) (PEG). This application of the calculation took into consideration the heterogeneity of microenvironments experienced by the probe in a sample containing vesicle aggregates of different sizes. Assuming that the aggregate size distribution was a delta function of the aggregate size, comparison of the calculated and observed lifetimes yielded an estimate of the vesicle aggregate size. For vesicles of varying compositions in the presence of dehydrating concentrations of PEG, this method suggested that only small aggreggates formed. For vesicles that could be demonstrated by other means not to have fused, the data were consistent with lipid transfer occurring only between the outer leaflets of two to four vesicles, even at high PEG concentrations. For vesicles that could be demonstrated to fuse by contents mixing and size changes, the fluorescence lifetime data were consistent with lipid transfer between both the inner and the outer leaflets of two to four fused vesicles. At very high PEG concentrations, where extensive rupture and large, multilamellar products were previously observed, the lifetime data were consistent with much more extensive lipid transfer within larger aggregates. The agreement of predictions made on the basis of lifetime measurements with other observations attests to the validity of the fluorescence lifetime method. In addition, the model and data presented here provide evidence that fusion occurs between small numbers of PEG-aggregated vesicles before the removal of PEG.     

Preparation of conductive nanocomposites based on poly (aniline-co- butyl 3-aminobenzoate) and poly (aniline-co-ethyl 3-aminobenzoate) by solution blending method

The polyaniline (PANI) is a widely studied conducting polymer due to its application in several devices such as biosensor, gas sensor etc. Known methods to produce PANI composites may be essentially reduced to two distinct groups: synthetic methods based on aniline polymerization in the presence of or inside a matrix polymer, and blending methods to mix a previously prepared PANI with a matrix polymer. Poly (aniline-co-butyl 3-aminobenzoate) (ANI-co-BAB) and poly (aniline-co-ethyl 3-aminobenzoate) (ANI-co-EAB) are prepared as conducting copolymers in nanoscale by chemical oxidation method under ultrasonic irradiation. The different molar ratio of aniline to butyl 3-aminobenzoate and ethyl 3-aminobenzoate are used in the preparation of copolymers. Conductive nanocomposites based on ANI-co-BAB or ANI-co-EAB with poly (styrene-alt-maleic acid) (PSMAC), and polystyrene are prepared by solution blending method. The obtained conductive composites formed films with good homogeneity and flexibility. The conductivity of the obtained nanocomposites is measured with a four-probe method. The electrical conductivity of the composites (ANI-co-EAB)/PSMAC/PS and (ANI-co-BAB)/PSMAC/PS are 24?×?10^?5?S?cm^?1 and 31?×?10^?5?S?cm, respectively. Our results show that the (ANI-co-BAB)/PSMAC/PS composite has more conductivity than (ANI-co-EAB)/PSMAC/PS composite. The copolymers and composites in nanoscale are characterized by FT-IR and ¹H NMR spectral data. The surface morphology was studied using SEM analysis. Also, their grain size is measured using XRD studies.     

The study of gamma irradiation effects on poly (glycolic acid)

We have investigated the effects of gamma irradiation on chemical structure, thermal and morphological properties of biodegradable semi-crystalline poly (glycolic acid) (PGA). PGA samples were subjected to irradiation treatment using a ⁶⁰Co gamma source with a delivered dose of 30, 60 and 90?kGy, respectively. Gamma irradiation induces cleavage of PGA main chains forming ～O?H₂ and ?H₂COO～ radicals in both amorphous and crystalline regions. The free radicals formed in the amorphous region abstract atmospheric oxygen and convert them to peroxy radicals. The peroxy radical causes chain scission at the crystal interface through hydrogen abstraction from methylene groups forming the ～?HCOO～ (I) radical. Consequently, the observed electron spin resonance (ESR) doublet of irradiated PGA is assigned to (I). The disappearance of the ESR signal above 190°C indicates that free radicals are formed in the amorphous region and decay below the melting temperature of PGA. Fourier transform infrared and optical absorption studies confirm that the groups are not influenced by gamma irradiation. Differential scanning calorimetry (DSC) studies showed that the melting temperature of PGA decreased from 212°C to 202°C upon irradiation. Degree of crystallinity increased initially and then decreased with an increase in radiation as per DSC and X-ray diffraction studies. Irradiation produced changes in the physical properties of PGA as well as affecting the morphology of the material.     

聚对苯撑及其烷氧基衍生物的能带研究

利用扩展Hückel分子轨道方法，运用BICON-CEDiT程序包计算了聚对苯撑及其系列烷氧基取代物的一维能带结构.计算结果表明：聚合物的能带结构在很大程度上受到杂原子、侧链等因素的影响，这与已知的实验结果相符；随着烷氧基侧链中C原子数的改变，聚合物的带隙呈现规律性变化.理论计算得到的带隙值与已有的实验观察值符合得相当好.     

Investigation of Pendant Group and Chain Segment Motions in P(MMA/BA) Copolymers by Thermally Stimulated Depolarization Current

Poly(methyl methacrylate/butyl acrylate) [P(MMA/BA)] copolymers (M_η ～2×10⁵) with different mass percentages of MMA were synthesized by the method of solution polymerization. Thermally stimulated depolarization current (TSDC) technique was used to investigate the effect of copolymerization on pendant group and chain segment motions. Three TSDC peaks were observed over the temperature range from 310 to 400 K. The highest temperature, ρ peak originates from the detrapping of trapped charge carriers. The lower temperature, α peak corresponds to the glass transition. The activation energy of the α relaxation decreases from 1.2 eV for PMMA to 0.98 eV for MMA(75)/BA(25). In the fitting process, another peak, β′, is separated on the low temperature side. The apparent energy barrier of the β′ for PMMA is 0.80 eV. The β′ relaxation is thought to correspond to the motion of pendant groups including intra‐ and inter‐molecular interactions. All three peaks move to lower temperatures with an increase in BA component, and the activation energy for the α and β′ relaxations also decreases with the increase of BA component in copolymers, indicating that the flexible side groups of BA have an effect of plasticization on the glass transition and motion of pendent groups. The temperatures of the α and β′ peaks of P(MMA/BA) copolymers follow the Fox equation. Fitting results gives the α peak at 238 K and β′ peak at 225 K for polybutyl acrylate (PBA).     

Structural and tribological responses of phenolphthalein poly(ether sulfone) on electron irradiation

The blocks of phenolphthalein poly(ether sulfone) (PES-C) were prepared by hot pressing. Then the blocks were irradiated with electron beams under N₂ atmosphere at room temperature. The structural and tribological responses of PES-C on electron irradiation were investigated. Results showed that partial degradation took place on the surface of PES-C after electron irradiation. Even so, the infrared spectra (FTIR) of PES-C after electron irradiation maintained much memory of the pristine sample, the reason for this might be due to the radiation-resistant property of PES-C and the less damage caused by the lower liner energy transfer of electron with respect to other ions. In addition, amorphous carbon and carbides formed on the surface of PES-C after electron irradiation. Friction and wear tests revealed that with increasing irradiation dose, it took more time for the friction coefficient to decrease from a higher value to a lower one and level off. And the wear rate decreased with the increase of irradiation dose. It was concluded that the variation of the tribological behavior of PES-C resulted from its structural responses on electron irradiation on the surface.     

Properties of acrylonitrile butadiene rubber (NBR)/poly(lactic acid) (PLA) blends and their foams

Abstract

Thermoplastic elastomers and their foams were prepared by blending elastomeric acrylonitrile butadiene rubber (NBR) and rigid poly(lactic acid) (PLA) with various PLA compositions ranging between 0 and 40%. The thermal and mechanical properties and the morphologies of the blends with various PLA contents were investigated through universal testing machine, differential scanning calorimetry, thermogravimetric analysis, and scanning electron microscope analysis. The rheological properties during gel formation were in situ monitored through the evolution of torque with curing time. Furthermore, the microcellular structures and physical properties of the NBR/PLA foams prepared using organic blowing agents were studied. The NBR/PLA blends showed a two-phase morphology made of a continuous NBR matrix and micron or submicron nodules and the tensile strength and modulus; also, hardness of the NBR/PLA blends increased with the increase of the added PLA content. While the foamed samples exhibited a similar cell structure and foaming ratio to that of the pure NBR, the cell formation was considerably reduced as the added PLA content exceeded 30%. We conclude that the mechanical properties of NBR thermoplastic elastomer as well as its foams can be controlled by a judicious introduction of rigid and biodegradable PLA.     

宏观电偶极子对聚丙烯铁电驻极体膜电荷储存及其动态特性的影响

利用栅控恒压电晕充电组合反极性电晕补偿充电法，研究了孔洞(单元电畴)内分布的空间电荷型宏观电偶极子的形成，及其增长对聚丙烯孔洞膜电极化期间的电流特性及电导率的影响. 借助等温表面电位衰减测量、开路和短路热刺激放电电流谱分析等，讨论了宏观电偶极子及其密度变化时的聚丙烯孔洞驻极体膜电荷储存稳定性及电荷动态特性. 实验结果说明：由电极化形成的宏观电偶极子的自身电场提高了聚丙烯孔洞驻极体膜的电导率，从而降低了驻极体膜电荷储存的稳定性. 对呈现弱极化强度的孔洞驻极体膜，以孔洞为畴结构基本单元内的宏观电偶极子，其两性空间电荷的大部分仅仅分别沉积在透镜状孔洞上下两壁的两端. 外激发脱阱电荷从脱阱位置的输运路径，主要是绕孔洞两边沿介质层迁移；而极化强度较高的样品，其两性电荷则分别分布在上下两壁的宽广区域内，脱阱电荷的大部分在驻极体电场驱动下从脱阱位置通过孔洞层间的介质层迁移并衰减.     

The Effect of Hydrophilic Bentonite Nanoclay on the Thermogelation Properties of Poly(N-isopropylacrylamide)-poly(ethylene glycol)-poly(N-isopropylacrylamide) Triblock Copolymer Aqueous Solutions

The effect of hydrophilic bentonite addition on the thermogelation properties of aqueous solutions of poly(N-isopropylacrylamide)–poly(ethylene glycol)–poly(N-isopropylacrylamide) (PNIPAM-PEG-PNIPAM) triblock copolymers of various compositions and molecular weights was investigated. Dynamic rheometry and differential scanning calorimetry (DSC) measurements showed that increasing concentrations of clay added to 20 wt.% polymer aqueous solutions caused a decrease of the temperature at which the viscosity starts increasing, while the temperature corresponding to the maximum endothermic effect due to the PNIPAM chain dehydration remained practically unchanged. The storage modulus, G′, increased with clay concentration for shorter PNIPAM chain triblock copolymers, while an opposite situation occurred in the case of the block copolymer with the longest PNIPAM block. For bentonite concentrations above 1 wt.%, G′ was larger than the viscous modulus, G″, at temperatures higher than the phase separation temperature, indicating a predominantly elastic character of the resulting composite hydrogels. These findings were explained through the presence of polymer–clay interactions occurring mainly through the PEG blocks.     

Crystallizaion and surface morphology of poly(vinylidene fluoride)/poly(methylmethacrylate) films by solution casting on different substrates

The dependence of surface structure of the poly(vinylidene fluoride) (PVDF)/poly(methylmethacrylate) (PMMA) films by solution casting on properties of seven substrates was investigated by wide angle X-ray diffraction (WAXD), Fourier transform infrared (FTIR), scanning electron microscope (SEM) and differential scanning calorimetry (DSC). It was revealed that the polyblend films obtained by casting onto each substrate contained exclusively β phase PVDF. Higher crystallinity of the film was obtained by casting onto ceramic, polytetrafluoroethylene (PTFE), copper (Cu), stainless steel and glass substrates than that by casting onto aluminium (Al) and polypropylene (PP) substrates, depending on the degree of close lattice matching. The surface crystalline structure of PVDF was strongly affected by the wettability of substrate. The largest size of PVDF spherulitic crystal structure with about 6 μm presented in the casting film grown at the air/solution interface on glass substrate, while the smallest spherulite size with about 3 μm was generated by casting onto PTFE, stainless steel and PP substrates. It implied that the higher surface tension the substrate had, the larger PVDF spherulite grew at the air/solution interface.