链缠结对等规聚苯乙烯结晶的影响

在1×10^－3～2×10^－5 g•mL^－1溶液浓度范围内, 用溶液雾化冷冻升华法制备了等规聚苯乙烯(i-PS)的单链、寡链非晶态聚集体. 随着溶液浓度降低, i-PS分子链团间的分离程度增大, 链间缠结随之减少, 因此冷冻升华制备的样品中单、寡链线团数目逐渐增多. DSC研究结果表明随着溶液浓度的降低, 冷冻升华样品的结晶温度逐渐降低; 等温结晶得到的晶粒熔点和结晶度降低. 由浓度为2×10^－5 g•mL^－1溶液制备的i-PS样品在468.3 K熔体结晶60 min后, 得到平均体积约为1.5×10⁴ nm³的单链晶粒. 用SEM观察到晶粒尺寸约为20～50 nm. 采用偏光显微镜(POM)测量了不同温度等温时i-PS单、寡链聚集体球晶的生长速率. 用Hoffmann理论进行了描述, 计算得到了i-PS单链聚集体熔体结晶片晶的端表面能(σ_e)为30.2 erg•cm^－2, 侧表面能(σ)为5.7 erg•cm^－2及单分子链折叠功(q)约为4.5×10^－13 erg•molecule^－1. 与文献值相比, 实验结果表明链缠结对聚合物结晶有很大影响.     

链缠结对高聚物热转变行为的影响

用冷冻升华方法,由等规聚苯乙烯、聚环氧乙烷的稀溶液制备单链、寡链附聚粒子．附聚粒子的热分析表明,冷结晶温度降低、结晶速度加快、晶体增厚明显．这些结果是因为附聚粒子没有或有很少链间缠结．附聚粒子形成较小尺寸的晶体,因而熔点较低,相应的热结晶温度移向低温．在平衡熔点以上放置短时间,链相互贯穿、缠结,又回复到本体的熔融、结晶行为     

二维红外相关光谱研究缠结对冷冻升华无规聚苯乙烯分子运动的影响

用冷冻升华法制备了浓度为1×10^－4 和2×10^－5 g/mL的单链无规聚苯乙烯(a-PS). 利用FTIR测试方法, 测定a-PS在等温处理时红外吸收峰的时间依赖性与温度依赖性, 研究样品中链缠结和链结构单元的堆积等因素对红外吸收峰的影响, 进而探讨链缠结对a-PS分子运动的影响. 同时, 也通过二维相关分析来研究a-PS等温实验过程中, 链缠结的变化情况以及官能团之间的变化顺序, 推断在a-PS等温时, 与链结构单元的堆积相联系的苯环振动首先发生, 其次才是与链缠结相关联的CH₂振动发生变化, 并由此确定缠结对冷冻升华a-PS分子运动的影响.     

燃料电池用侧链型磺化聚砜质子交换膜的性能

在制备氯甲基化聚砜(CPS)的基础上,以1,2-二羟基苯-3,5-二磺酸钠为试剂,通过亲核取代反应制备一种侧链末端为磺酸基团的侧链型磺化聚砜(PS-BDS),并采用溶液浇注法制备相应的质子交换膜(PEM),研究温度对PEM性能的影响规律。 结果表明,由于亲水基团远离疏水聚合物主链,该PEM能够形成亲水微区远离疏水微区的相分离结构,亲水区域对主链的影响较小,该PEM在高磺化度下仍能保持较好的尺寸稳定性,随着温度的升高,PEM的吸水率(WU)、吸水溶胀率(SW)和质子传导率(PC)升高,其中PS-BDS-4(离子交换容量为1.57 mmol/g)在25和85 ℃时的SW仅为22.1%和55.0%,甲醇的渗透率(DK)仅为10.17×10^-7 cm²/s,低于商业化的Nafion115(16.8×10^-7 cm²/s)和Nafion117(23.8×10^-7 cm²/s),表现出很好的综合性能。     

几种聚合物分子间激基缔合作用的研究

作者合成并纯化了聚[对苯二甲酸(聚四亚甲基醚二醇)酯](PPTMGTP)、聚[2、6-萘二甲酸(聚四亚甲基醚二醇)酯](PPTMGNDC)和聚[2,6-萘二甲酸(环氧丙烷-四氢呋喃共聚醚二醇)酯](PCPEGNDC)等三个新聚合物,测定了它们的凝胶渗透色谱和数均分子量,对它们在良溶剂和不良溶剂溶液中的荧光进行了研究, 严格地用实验证明了PPTMGTP溶液中链内非相邻激基缔合作用的存在, 进一步以链内非相邻攀基缔合作用为探针研究了高分子在溶液中的形态随溶剂和浓度的变化, 用激基缔合物荧光相对强度的浓度依赖性测出高分子线团开始感觉到邻近有其它线团存在而收缩的浓度C_s(PPTMGNDC氯仿溶液的C_s = 2.61×10^-3g/ml, PPTMGNDC乙酸乙醋溶液的C_s =4.0×10^-2g/ml)。首次提出用C.划分高分子溶液稀浓区和亚浓区的界限的新欢点,以链内非相邻和链间激基缔合作用为探针确定了高分子溶液链段空间密度趋于均一的浓度C⁺(PPTMGNDC级仿溶液C⁺ = 7.02×10^-2g/ml),认为C⁺是高分子溶液由亚浓区到浓区的转变浓度。     

基于金纳米棒-壳聚糖复合膜的葡萄糖生物传感器

本文采用金纳米棒-壳聚糖复合膜固定葡萄糖氧化酶构建电流型葡萄糖生物传感器.通过电化学交流阻抗法和循环伏安法对酶膜状态进行了表征,得到了相应的等效电路和动力学参数.实验结果表明,金纳米棒-壳聚糖复合膜可以辅助电子传递,提高电极的电流响应,并使生物传感器的使用温度范围有很大的扩展.此传感器表现出对葡萄糖溶液浓度的优良响应,线性范围在2.78×10^-5mol/L—2.22×10^-3mol/L,响应灵敏度约为7.819μA·cm^-2(mmol/L)^-1,表观米氏常数为10mmol/L.本工作还研究了温度和溶液pH值对电极电流响应的影响.     

应用纳米磁性球电化学检测特定序列DNA

采用分散聚合法制备纳米磁性羧基球,利用化学偶联法将末端修饰氨基的寡聚核苷酸固定在纳米磁性球表面,制成新型核酸探针,该探针可特异性结合目标单链寡聚核苷酸.在磁场作用下,将纳米磁珠与本体溶液分离并富集在电极表面,以中性红为嵌合指示剂,用示差脉冲伏安法测定杂交结果.经过条件优化,本法测定DNA的浓度线性范围为1.0×10^-6～5.0×10^-9mol/L,检出限为8.6×10^-10mol/L.     

链解缠结聚对苯二甲酸乙二酯的结晶行为研究

采用冷冻萃取聚对苯二甲酸乙二酯(PET)溶液(0.1～10g/dL7种不同浓度,3种不同性能溶剂)的方法制备了解缠结PET试样.与链相互穿透且缠结的熔体骤冷试样相比,解缠结PET试样的结晶能力明显增强,且随着制样溶液浓度的降低,链间解缠结程度增加,PET的结晶能力逐渐增强,有序结构含量明显增加,但是如果制样溶液浓度太低,溶液中链间距离太大,则又不利于萃取过程中链间的有序堆砌而结晶.采用接触浓度c*附近的溶液,既可确保链间的有效解缠结又有利于链间的有序堆砌而结晶.PET的结晶能力甚至还受制样所用溶剂性能的影响,这是因为溶剂性能影响了溶液中链间的相互作用以及链的解缠结程度.     

溶致凝聚过程中分子链构象的演变

详细讨论了稀溶液、亚浓溶液、浓溶液和极浓溶液中分子链构象的演变,考察了在溶致凝聚过程中分子链的链间相互作用、关联作用和分子链尺寸的变化规律,给出了排除体积的严格定义,引入热关联效应、长程关联效应和全高斯链浓度等概念。指出在不同浓度溶液中,分子链在不同尺度上构象状态不同;在从孤立单链态(良溶液中)向多链聚集态的溶致凝聚过程中,单链的尺寸一直在收缩,由Flory尺寸RF缩小至无扰尺寸R0。这是大分子凝聚过程的一个特点。     

富含胞嘧啶单链DNA-银纳米簇荧光探针用于S1核酸酶的灵敏检测

以富含胞嘧啶（C）的单链DNA为模板合成银纳米簇,将其作为功能化探针,建立了一种无标记荧光检测S1核酸酶的方法.S1核酸酶可以特异性识别单链DNA,在最适的酶催化反应条件下,可将其降解为单核苷酸或寡核苷酸片段.当S1核酸酶不存在时,富含C的单链DNA可以有效地合成荧光银纳米簇;当S1核酸酶存在时,单链DNA模板被特异性识别并降解,导致无法形成银纳米簇,使体系荧光信号降低.实验结果表明,银纳米簇的荧光强度随着S1核酸酶浓度的增加而降低.在优化的条件下,体系荧光信号（F/F₀）与S1核酸酶的浓度在5.0×10^-5~4.0×10^-3 U/μL范围内呈线性关系,检出限为2.0×10^-6 U/μL.该荧光探针选择性好,可用于RPMI 1640细胞培养基中S1核酸酶的检测,回收率达到91.8%~109.5%.     

Morphology of homogeneous copolymers of ethylene and 1‐octene. III. Structural changes during heating as revealed by time‐resolved SAXS and WAXD

The structural changes of two linear polyethylenes, LPEs, with different molar mass and of two homogeneous copolymers of ethylene and 1‐octene with comparable comonomer content but different molar mass were monitored during heating at 10 °C per minute using synchrotron radiation SAXS. Two sets of samples, cooled at 0.1 °C per minute and quenched in liquid nitrogen, respectively, were studied. All LPEs display surface melting between room temperature and the end melting temperature, whereas complete melting, according to lamellar thickness, only occurs at the highest temperatures where DSC displays a pronounced melting peak. There is recrystallization followed by isothermal lamellar thickening if annealing steps are inserted. The lamellar crystals of slowly cooled homogeneous copolymers melt in the reverse order of their formation, that is, crystals melt according to their thickness. Quenching creates unstable crystals through the cocrystallization of ethylene sequences with different length. These crystals repeatedly melt and co‐recrystallize during heating. The exothermic heat due to recrystallization partially compensates the endothermic heat due to melting resulting in a narrow overall DSC melting peak with its maximum at a higher temperature than the melting peak of slowly cooled copolymers. With increasing temperature, the crystallinity of quenched copolymers overtakes the one of slowly cooled samples due to co‐recrystallization by which an overcrowding of leaving chains at the crystal surfaces is avoided. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 1975–1991, 2000     

Polydispersity of ethylene sequence length in metallocene ethylene/α‐olefin copolymers. II. Influence on crystallization and melting behavior

In this work, crystallization and melting behavior of metallocene ethylene/α‐olefin copolymers were investigated by differential scanning calorimetry (DSC) and atomic force microscopy (AFM). The results indicated that the crystallization and melting temperatures for all the samples were directly related to the long ethylene sequences instead of the average sequence length (ASL), whereas the crystallization enthalpy and crystallinity were directly related to ASL, that is, both parameters decreased with a decreasing ASL. Multiple melting peaks were analyzed by thermal analysis. Three phenomena contributed to the multiple melting behaviors after isothermal crystallization, that is, the melting of crystals formed during quenching, the melting‐recrystallization process, and the coexistence of different crystal morphologies. Two types of crystal morphologies could coexist in samples having a high comonomer content after isothermal crystallization. They were the chain‐folded lamellae formed by long ethylene sequences and the bundlelike crystals formed by short ethylene sequences. The coexistence phenomenon was further proved by the AFM morphological observation. © 2002 Wiley Periodicals, Inc. J Polym Sci Part B: Polym Phys 40: 822–830, 2002     

Mechanisms of reorganization of lamellae in syndiotactic polystyrene

The multiple melting behavior of syndiotactic polystyrene (sPS) and its possible mechanisms via preexisting lamella types and/or scanning-induced lamellar reorganization were investigated by using X-ray diffraction, DSC, and scanning electron microscopy. Melt-crystallized sPS samples, upon DSC scanning, exhibited three melting peaks (I, II, III). A morphological analysis showed that flat-on lamellae develop first, which yield P-I and P-II melting, and during scanning recrystallize to thickened edge-on lamellae with a P-III melting peak. Upon scanning, melting of P-I (crystal of the lowest melting peak) is followed by repacking into thickened P-III crystal, the lamella of which also reoriented to a perpendicular orientation. The P-II crystal, however, melts at temperatures too close to the melting temperature of P-III; thus, during scanning up, the P-II crystal simply melts without sufficient time to repack into the thickened P-III crystal. In addition to the P-III crystal species that can be added by melting P-I and repacking to P-III, it is believed that preexistence of different lamella crystals was jointly responsible for the multiple melting. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 3210–3221, 2000     

Relationship between Localization of PBSU in Interlamellar/Interfibrillar Regimes and Double Peaks in DSC/SAXS in its Blend with PVDF

In this work, phase segregation and localization of PBSU have been investigated with the combination of SAXS and DSC in its blend with PVDF. After stepwise crystallization of PVDF and PBSU, there are double melting peaks of PBSU in DSC and double scattering peaks in SAXS. It has been demonstrated that double peaks can be attributed to the localization of PBSU in interlamellar/interfibrillar region in pre-formed PVDF crystal framework. In the case of low content of PBSU in blend, PBSU is trapped into the interlamellar region of PVDF crystals, resulting in the alternating lamellae crystal of them and the first peak (with low-q) in SAXS. The enhanced confinement effect produces thinner PBSU lamellae, corresponding to the lower melting temperature in DSC. Upon increasing its content in blend, some PBSU segregates in interfibrillar regions in addition to the enrichment in interlamellar regions of PVDF crystal framework. The larger space and higher concentration of PBSU in interfibrillar-regions contribute to periodic lamellae structure of PBSU with higher thickness, which is the reason for the second peak (with high-q) in SAXS and DSC. Our results not only clarify the relationship between localization of PBSU in interlamellar/interfibrillar regions and double peaks in DSC/SAXS, but also provide a novel strategy to detect the interlamellar and interfibrillar segregation of low-T_m component in miscible crystalline/crystalline blend.

     

聚环氧乙烷的双层片晶

聚环氧乙烷(M_n=7000)的双层片晶形态用透射电镜和差示扫描量热计进行了研究。在结晶温区54—56℃,现察到双层片晶,高于这个温区,同时看到双层片晶及单层片晶,低于这个温区,只看到单层片晶。双层片晶的熔点稍高于单层片晶。根据非整数次折迭链晶向整数次折迭链晶的转变,讨论了双层片晶和单层片晶的生长过程。在双层片晶界面上的H键降低了表面自由能,这是形成双层片晶的主要原因。     

偏氟乙烯/三氟氯乙烯无规共聚物的结晶

用示差扫描量热法(DSC)、广角X射线衍射(WAXD)和傅里叶红外光谱(FTIR)研究了偏氟乙烯/三氟氯乙烯单体摩尔比为1:4的无规共聚物的结晶与晶体结构.结果表明,该无规共聚物属于半结晶型聚合物.在333～353K温度范围内退火,片晶逐渐完善、增厚,熔点和结晶度均随着退火时间的延长而升高.于353K退火时,由DSC结果计算得到片晶厚度约4.68nm.在333K退火时得到共聚物的最大结晶度约为14%.WAXD测试结果表明,沿晶粒(101)晶面的面间距为0.55nm,垂直于(101)衍射晶面方向上的晶粒平均尺寸为5.86nm.     

聚L-乳酸/4,4'-二羟基二苯硫醚共混物的分子间相互作用及结晶和熔融行为

利用红外吸收光谱(FTIR)研究了聚乳酸(PLLA)/4,4'-二羟基二苯硫醚(TDP)熔融共混物的分子间相互作用,结果表明,PLLA的羰基与TDP的羟基之间形成了分子间氢键.通过差示扫描量热(DSC)研究了共混物的玻璃化转变行为及非等温结晶和熔融行为.结果表明,样品的玻璃化转变温度(Tg)随TDP含量的增加呈线性下降.共混物的熔融结晶温度(Tc)、结晶焓(ΔHc)、熔融温度(Tm)及熔融焓(ΔHm)均随TDP含量的增加呈下降趋势,而冷结晶温度的变化趋势则相反.当TDP达到40%(质量分数)时,共混物的DSC曲线既未出现结晶峰,也未出现熔融峰,表明该样品已完全成为非晶态物质.广角X射线衍射(WAXD)分析结果表明,TDP的加入未改变PLLA的晶型,但导致其晶面间距变大,晶体结构变得松散.因此共混物熔点的下降归因于分子间氢键的形成降低了PLLA分子链的运动能力及晶体的紧密程度而非晶型的改变.     

Multiple Endothermic Peaks Resulted from Different Crystal Structures in an Isomorphous Copolymer Poly(3-hydroxybutyrate-co-3-hydroxyvalerate

The multiple endothermic peaks of poly(3-hydroxybutyrate-co-3-hydroxyvalerate)(P(HB-co-HV)) in differential scanning calorimetry(DSC) results, as one representative phenomenon of polymer with unique cocrystallization behavior, were generally considered as the results of melting/recrystallization. In this study, wide angle X-ray diffraction(WAXD) and small angle X-ray scattering(SAXS) experiments were conducted to analyze the phenomena of multiple endothermic peaks in DSC results. The results of these analyses indicated that the multiple endotherms were mainly caused by different lamellae structures. For P(HB-co-HV) with lower HV content, it was comprised of two structures of HV total exclusion and HV partial inclusion in the crystal lamellae. For P(HB-co-HV) with higher HV content, it was also comprised of two structures of HV total inclusion and HV partial inclusion in the crystal lamellae. However, only structure with HV partial inclusion in the crystal lamellae remained existing after first melting peak for all samples.     

单链和寡链等规聚苯乙烯聚集体的结晶行为

自1960年Hoffman等提出聚合物结晶成核理论以来,人们对聚合物结晶生长速率、片晶的侧向尺寸随过冷度的变化等现象成功地进行了理论描述．1997年,Hoffman等对聚合物结晶成核理论进行修正,将de Gennes的聚合物“蛇行”概念。引入表面成核理论,通过对单根分子链从过冷熔体“卷绕”到晶体前沿所需的时间进行估算,其结果远远低于Flory预言时间约3～5个数量级,据此,Hoff-man认为,在聚合物结晶过程中,分子链在强迫稳态下的“蛇行”运动有足够的时间解缠结和结晶。     

用正电子湮没谱研究聚酯型聚氨酯的微观结构和自由体积特性

用正电子湮没谱研究了两类分别由聚己二酸丁二醇酯多元醇和聚ε 己内酯多元醇合成的线型聚酯型聚氨酯 (PBU和PCU)在 140～ 36 0K温度范围内的结构转变和自由体积特性 .研究结果表明 ,两类聚氨酯(PU)在 140～ 36 0K温度范围内 ,都存在三个转变点 ,其中较低温度的转变 (约 2 0 0K)对应于PU中软段的玻璃化转变温度 (Tg) ,2 75K处的转变可能与样品吸附少量水分有关 ,较高温度的转变 (约 310K) ,对于PBU而言对应于软段结晶的熔点 ,而对于PCU则与在无序的硬段中混入一定量的软段后形成的相容区的Tg 有关 .当温度低于PU软段的Tg 时 ,两类PU的自由体积尺寸和浓度都随温度升高而增大 .当温度高于软段的Tg 但低于2 75K时 ,自由体积尺寸较快地增加 ,而自由体积浓度保持不变 .温度高于 2 75K并低于软段的熔点或硬段 软段相容区的Tg 时 ,自由体积尺寸增加速度最快 ,自由体积浓度却保持同样的数值 .当温度进一步升高时 ,自由体积尺寸和浓度都随温度增大而增加 .最后研究了这两类PU的自由体积分布与温度的关系 .所有这些实验现象均与大分子链的运动有关 ,并与通过DSC和WAXD表征的材料的形态一致