聚碳酸酯与苯乙烯-丙烯腈共聚物共混体系相容性及其对光学性能的影响

利用分子内链段排斥性相互作用理论研究了聚碳酸酯 (PC) 苯乙烯 丙烯腈共聚物 (SAN)共混体系中组份分子量及SAN共聚比例对体系相容性的影响规律 ,确定了获得均相的PC SAN共混体系的条件 ,考察了体系相容性与光学性能之间的关系 .通过实验获得了均相的PC SAN共混物 ;研究结果表明PC聚合度为 90、SAN聚合度为 3 0的PC SAN(S体积含量为 68%)体系共混比在 60∶40附近时体系的双折射能够实现补偿 ,紫外透光率达到 70 %.     

单分散功能化聚硅氧烷微球的制备及其应用

采用悬浮聚合法以正硅酸乙酯(TEOS)和γ-甲基丙烯酰氧基丙基三甲氧基硅烷(MPS)为主要原材料,制备表面功能化的单分散聚硅氧烷微球。采用扫描电镜(SEM)、动态光散射(DLS)和红外光谱(FT-IR)等分析手段分别对功能性微球的微观形貌、粒径分布和微观结构进行表征。将这种表面功能性的单分散聚硅氧烷微球按照0.4%的添加量加入光学级聚碳酸酯(PC)树脂中,可制备出透光率75.6%、雾度94.6%性能优良的光散射材料。     

小角光散射在线系统研究多相聚合物双螺杆挤出过程中的相尺寸--非相容PE/PA1010体系

利用可视化双螺杆挤出机———光散射在线采集与分析系统对不相容聚合物体系聚乙烯 尼龙 10 10(PE PA10 10 )双螺杆挤出过程进行了在线分析 .相尺寸由Debye理论中的相关距离ac,平均弦长L ,以及分散相平均直径D描述 ,给出了几种参数表征适用的范围 .由在线光散射计算出的平均弦长Lscatt、分散相平均粒径Dscatt与电镜照片计算出的平均弦长LSEM 、分散相平均粒径DSEM 作了比较 ,两者比较符合 .结果表明 ,分散相颗粒尺寸沿螺杆挤出方向逐渐变小 ;随着低组分含量 (PA10 10≤ 5 0 % )的增加 ,分散相颗粒尺寸变大 ,在组成比为 70 30和 6 0 4 0时出现双连续相     

流场中聚乳酸/聚碳酸酯共混体系的酯交换反应及其形态结构研究

选用钛酸四丁酯作为聚乳酸(PLA)/聚碳酸酯(PC)的酯交换反应催化剂,通过透射电子显微镜(TEM)和核磁共振氢谱(1H-NMR)研究了流场中不同组分比的PLA/PC共混体系酯交换反应机理及酯交换反应对不同组分比的共混体系相形态的影响.研究发现,无论在PLA/PC共混体系中是否含有催化剂,酯交换反应次数、参与酯交换反应的PC的含量、生成的共聚物中PC链段的含量及生成的共聚物的总质量和总摩尔数均随组分中PLA含量的增加而增加,催化剂的加入更拉大了这种差距.主要原因是与PC作为连续相相比,当PLA作为连续相时PLA链段沿界面的取向程度更高,从而导致进行多次酯交换反应的几率增加.添加催化剂后,影响酯交换反应的主导因素发生变化,从而导致PLA/PC 30/70体系界面反应的机理发生改变.钛酸四丁酯有效地促进了PLA/PC体系的酯交换反应,使分散相的尺寸都得到不同程度降低,尤其当PLA为连续相时催化产生的共聚物的总摩尔数更多,从而使PLA为连续相时的分散相粒径较PC为连续相时降低的更多.     

聚碳酸酯/碳纳米管复合热电材料的制备与性能研究

本文首先通过溶液混合法将碳纳米管(CNTs)分散到聚碳酸酯(PC)基体中,然后将获得的PC/CNT絮状物通过高温模压的方法制备了一种柔性的高热电性能PC/CNT复合材料。PC/CNT复合材料断面形貌分析表明,CNTs均匀地分散在PC基体中。此外,PC/CNT复合材料的导电性随着CNTs含量的增加而急剧增加,而Seebeck系数几乎保持恒定,使得材料的功率因子随着CNTs含量的增加而快速增加,最大功率因子达到4.6μW·m^-1·K^-2。     

聚(ε-己内酯)/苯乙烯-丙烯腈共聚物共混物的形态研究

本文研究了聚(ε-己内酯)(PCI/苯乙烯-丙烯腈共聚物(SAN)共混物的形态。采用差示扫描量热计(DSC)测量了PCL/SAN共混物中的PCL结晶度随着SAN含量的增加而下降;当SAN浓度达到60wt％。以上时,PCI的结晶度趋于零。通过偏光显微镜可以观察到在含高浓度PCI的共混物中,PCL是以球晶形式存在的。样品是由PCL球晶充满的,但是随着SAN含量的增加,PCL球晶半径减小,球晶结构逐渐变得不规整,而X-射线衍射测试了不同组成的PCL/SAN共混物中PCL的晶胞参数没有改变,说明SAN没有进入到PCL的晶胞内。以小角X-射线散射结果发现PCI片晶之间的距离随着SAN含量的增加而增大。以上说明SAN分子与没有结晶的PCL形成无定形相夹在PCL的片晶之间。     

亚微米级聚苯乙烯/聚硅氧烷核壳粒子的制备及其应用

以乳液聚合制备的聚苯乙烯乳液为种子,加入甲基三甲氧基硅烷(MTMS)水解溶液进行缩聚反应,合成亚微米级聚苯乙烯/聚硅氧烷核壳粒子,并以此作为光散射剂添加至聚甲基丙烯酸甲酯(PMMA)树脂中,制备了光散射材料;考察了亚微米级核壳粒子添加在PMMA树脂中的分散性。结果表明:经过双螺杆剪切作用的挤出加工后,可以实现核壳粒子在PMMA树脂中的良好分散。核壳粒子可以大幅度提高PMMA的雾度,当聚苯乙烯/聚硅氧烷核壳粒子(NS82)的含量为1%时,制得的PMMA样片(厚度为2 mm)的雾度为89%,透光率为69%,有效光散射系数为61%。     

基于异甘露醇和间苯二甲酸的光学共聚酯的合成及性能表征

合成了聚(对苯二甲酸乙二醇酯-共-对苯二甲酸异甘露醇酯-共-间苯二甲酸乙二醇酯-共-间苯二甲酸异甘露醇酯)(PEIIT).通过差示扫描量热分析(DSC)、紫外-可见-近红外光谱(UV-Vis-NIR)、X射线衍射(XRD)、偏光显微镜(POM)球晶培养等分析方法研究了PEIIT的结晶性能、光学性能及热性能.阐述了增加四元共聚酯PEIIT中间苯二甲酸结构单元的含量可以有效降低其结晶度和结晶速率的具体机制.间苯二甲酸结构单元含量的增加使PEIIT链段运动过程中的空间位阻增大,结晶能力降低,其冷结晶温度逐渐升高,热结晶温度逐渐降低直至不再有热结晶现象产生.由于结晶程度的降低,PEIIT的雾度可以完全降为零,并且透光率可以达到90.7%.同时发现了造成PEIIT透光率降低的吸光因素,黄变程度增加使330~550 nm波长的蓝紫光被PEIIT吸收,导致其透光率受到影响.PEIIT的熔点受间苯二甲酸含量变化影响较大,但仍保持了良好的耐热分解性能.     

SEOS/h-PEO共混物薄膜的微观分相结构

采用透射电子显微镜(TEM)观察由结晶性均聚物聚氧乙烯(h-PEO)与半结晶性嵌段共聚物聚苯乙烯-嵌-聚氧乙烯-嵌-聚苯乙烯(SEOS)组成的干、湿刷共混物薄膜结构.结果表明:4种共混系统的薄膜结构均由嵌段PEO和PEO均聚物组成球形PEO分散相;随着均聚物含量的增加,PEO分散相尺寸逐渐增大;当均聚物质量分数增大到33.3%时,在聚苯乙烯(PS)连续相中形成了类似胶束的"核-壳"结构.     

纳米SiO_2对PDMS/PIB不相容共混物在低剪切速率下凝聚行为的影响

借助在线剪切-显微装置研究了简单剪切流场下疏水纳米二氧化硅(SiO2)粒子对聚二甲基硅氧烷/聚异丁烯(PDMS/PIB=90 wt%∶10 wt%)不相容共混物实时结构演变过程的影响.研究表明,分散相尺寸的大小及其分布由粒子含量和剪切速率共同决定.少量纳米SiO2的加入能够抑制PIB分散相的凝聚,分散相的尺寸随着纳米SiO2含量的增大而减小,并且呈现出双峰分布.但随着SiO2粒子含量的进一步增加,分散相尺寸的双峰分布现象逐渐消失.SiO2的加入还导致PIB分散相对剪切速率的依赖性降低.当SiO2粒子含量低于2.5wt%时,较高的剪切速率凝聚得到的分散相的尺寸较大;当SiO2粒子含量超过2.5 wt%后,低速和高速剪切速率下凝聚得到的分散相尺寸基本相同.粒子的包覆、分散相的破碎和凝聚是出现以上现象的根本原因.     

Effect of PBT molecular weight and reactive compatibilization on the dispersed‐phase coalescence of PBT/SAN blends

Poly(butylene terephthalate) (PBT)/styrene‐acrylonitrile copolymer (SAN) blends were investigated with respect to their phase morphology. The SAN component was kept as dispersed phase and PBT as matrix phase and the PBT/SAN viscosity ratio was changed by using different PBT molecular weights. PBT/SAN blends were also compatibilized by adding methyl methacrylate‐co‐glycidyl methacrylate‐co‐ethyl acrylate terpolymer, MGE, which is an in situ reactive compatibilizer for melt blending. In noncompatibilized blends, the dispersed phase particle size increased with SAN concentration due to coalescence effects. Static coalescence experiments showed evidence of greater coalescence in blends with higher viscosity ratios. For noncompatibilized PBT/SAN/MGE blends with high molecular weight PBT as matrix phase, the average particle size of SAN phase does not depend on the SAN concentration in the blends. However noncompatibilized blends with low molecular weight PBT showed a significant increase in SAN particle size with the SAN concentration. The effect of MGE epoxy content and MGE molecular weight on the morphology of the PBT/SAN blend was also investigated. As the MGE epoxy content increased, the average particle size of SAN initially decreased with both high and low molecular weight PBT phase, thereafter leveling off with a critical content of epoxy groups in the blend. This critical content was higher in the blends containing low molecular weight PBT than in those with high molecular weight PBT. At a fixed MGE epoxy content, a decrease in MGE molecular weight yielded PBT/SAN blends with dispersed nanoparticles with an average size of about 40 nm. © 2010 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys, 2010     

Small-angle scattering of polarized light. II. experiments with isotropic spheres

New experimental measurements are reported of small-angle polarized and depolarized light scattering from almost monodisperse isotropic, spherical particle, polystyrene latexes. The shape and intensity distribution of the scattering patterns is shown to compare closely with the calculated patterns based on the exact Mie scattering theory from a single sphere.     

The fabrication of novel optical diffusers based on UV-cured polymer dispersed liquid crystals

Polymer dispersed liquid crystals (PDLCs) with different sizes of the LC droplets are prepared based on the ultraviolet (UV) light curable acrylate monomers/LCs composites to fabricate the optical diffuser films. To acquire light diffusers with high optical performance, the effects of the monomer structure and the UV light intensity on the micro-structure of the PDLC films are studied. Results show that the PDLC films could exhibit a strong light scattering at the premise of maintaining high transmittance in the visible region. As the LC droplets are spherically dispersed in the polymer networks, when the size of LC droplets is about 3.0 μm, the haze can reach 88.5% and the transmittance is nearly 90.0%, which can be used as a bottom diffuser film. While when the size of LC droplets is about 10.0 μm, the haze and transmittance are 39.2% and 90.2%, respectively; hence, it can be a good choice for a top diffuser film. With the advantages of simple preparation, roll-to-roll industrial production and tunable optical properties, it is supported that the films based on UV-cured PDLC films can be applied as outstanding optical diffuser films in the liquid crystal display industry.     

Crystallization behavior and hydrophilicity of poly (vinylidene fluoride) (PVDF)/poly (styrene-<Emphasis Type="Italic">co</Emphasis>-acrylonitrile) (SAN) blends

Poly (styrene-co-acrylonitrile) (SAN) is a hydrophilic non-crystalline copolymer, which is initially used in this paper to improve the hydrophilicity of poly (vinylidene fluoride) (PVDF). Investigation of the crystallization behavior of PVDF/SAN blends showed that the samples presented only α phase regardless of SAN content as cooling from the melt. A double-melting phenomenon was related to the perfection or crystal size of PVDF crystals. As the SAN content is increasing, crystallization of PVDF was limited, leading to a decreased crystallinity and lamellar growth. Besides, the hydrophilicity of PVDF was improved by blending with SAN. The sample containing 70 wt.% SAN performed a similar surface property of the neat SAN owing to the besieging of the PVDF phase by SAN. Observed from the cross section of the blends, PVDF/SAN blends were partially miscible with less than 50 wt.% SAN addition. As the SAN content was more than 50 wt.%, the crystalline PVDF particles clearly dispersed in the amorphous matrix.     

SiO_2粒子对PMMA/SAN共混体系相分离行为的影响

采用小角激光光散射(SALLS)并结合动态流变学方法,考察了气相法二氧化硅(SiO2)粒子的加入对聚甲基丙烯酸甲酯/苯乙烯-丙烯腈无规共聚物(PMMA/SAN)共混体系相行为的影响,得到了添加SiO2粒子前后的相图,发现SiO2粒子对基体相行为的影响与基体的组成有关.对PMMA/SAN(60/40)体系,加入SiO2粒子后相分离温度上升,但并未改变相分离机理,仍为亚稳单相分解过程(spinodal decomposition,SD);而对于PMMA/SAN(30/70)体系,加入SiO2粒子后却降低了体系的相分离温度.该现象可能是SiO2粒子和基体组分界面间组成与PMMA/SAN共混物基体组成的差异造成的.     

Cavity ring-down spectroscopy measurement of single aerosol particle extinction. II. Extinction of light by an aerosol particle in an optical cavity excited by a cw laser

The authors present an analytical derivation of the scattered power from a spherical, homogeneous, nonabsorbing particle in a plane standing wave. The scattered power changes significantly with the position of the particle with respect to the peaks and nodes of the standing wave, even for particles whose diameters are many times the wavelength of the light. The analysis is applicable to continuous-wave cavity ring-down spectroscopy on aerosol particles, and the structure of the standing wave is expected to affect both the measured ring-down time and the shape of the ring-down trace. The dependence of the extinction on the phase of the standing wave at the location of the particle is captured in a parameter zeta which connects the current treatment to standard Mie scattering theory. Methods for calculating zeta are presented.     

Chromatography of Suspensions - Analytical Corrections for Axial Dispersion

Abstract

An analytical method is proposed to correct the signal from a turbidity detector for axial dispersion in the chromatography of particle suspensions. An earlier analytical method due to Hamielec and Singh [1] is limited to light scattering in the Rayleigh regime. The solution reported herein is derived using the more general Mie light scattering theory and enables the correction of various moments of the particle diameter frequency distribution function. The axial dispersion phenomenon is described by the well known integral equation where the instrumental spreading function is assumed Gaussian. The solution is applicable for both linear and nonlinear particle diameter-retention volume calibration curves.