结晶对等规立构聚甲基丙烯酸甲酯辐射消旋和辐射裂解的影响

 本文通过核磁氢谱、DSC和分子量测定,研究了结晶对等规立构聚甲基丙烯酸甲酯辐射消旋和辐射裂解的影响.分子量测定的结果表明,等规立构聚甲基丙烯酸甲酯结晶后,其辐射裂解反应减弱,裂解G值减小将近一半.核磁氢谱测定辐照试样的空间立构变化结果为:随着辐照剂量的增加,等规立构逐渐变为无规立构和间规立构,其变化规律相似于非晶试样.结果还表明,晶区的消旋反应比裂解反应更为显著.DSC测得的试样熔点,随着辐照剂量的增加而急剧下降,由Flory结晶熔化理论计算得晶区的辐射破坏G值为8.8.该值远大于聚乙烯晶区的破坏G值.     

分子活动性对iso-PMMA辐射裂解和消旋的影响

以全同立构聚甲基丙烯酸甲酯(iso-PMMA)为对象, 用核磁共振谱和分子量测定等手段, 研究了不同物理状态, 即无定型固态, 结晶态和稀溶液状态下的辐射裂解和辐射消旋反应. 结果表明, 在稀溶液状态下辐照, 其裂解反应最强, 而消旋反应最弱; 结晶状态下辐照, 则裂解反应最弱而消旋反应最强. 这充分说明了分子的活动性对反应的影响, 进一步验证了前已提出的高分子链断裂-重合-消旋的平衡反应机理.     

聚甲基丙烯酸甲酯辐射裂解和消旋的空间立构效应

本文研究了三种不同空间立构聚甲基丙烯酸甲酯的辐射效应,提出裂解过程是一种裂解与重合的动态平衡过程。分子量降低和消旋作用对温度的依赖性,是由于分子运动和笼罩效应以及重合的空间位阻效应所致。辐照温度愈高,裂解产额愈大。相同条件下辐照,全同立构比无规立构试样的裂解产额更大。 全同立构聚甲基丙烯酸甲酯辐照后,不仅分子链断裂,而且空间立构也发生很大变化。随着辐照剂量的增加,全同立构含量逐渐减少,而无规立构含量和间同立构含量却逐渐增加。     

结晶聚合物的辐照效应——Ⅰ.尼龙-1010的聚集态结构对其辐射化学反应的影响

本文用DSC,WAXD,ESR和介电谱以及凝胶分数测定等技术,研究Nylon-1010的聚集态对γ-辐射化学反应以及辐照后热处理结果的影响。结果表明,辐照Nylon-1010的交联与裂解反应主要发生在非晶区或结晶表面,进一步证明了非晶区也是辐射后交联和后裂解主要反应区。     

聚丙撑碳酸酯的辐射效应

研究了室温条件下聚丙撑碳酸酯(PPC)在钴-60和电子加速器辐照过程中的响应行为。结果表明,聚丙撑碳酸酯是一种辐射裂解型聚合物,其分子量随着辐射剂量的增加而减小。1mm厚PPC片材在室温和N2气保护条件下,其裂解G值为Gs,γ-ray=10.81;Gs,EB=4.9。不同的裂解G值表明,O2气在聚丙撑碳酸酯的辐射裂解过程中有重要影响。红外光谱研究表明,辐射后聚丙撑碳酸酯在3474cm-1处的峰宽峰高增加,表明其裂解后端—OH基增加。由于裂解作用,辐射后聚丙撑碳酸酯的抗张强度和断裂伸长率均下降。在通常的辐射消毒剂量范围内(25~50kGy),PPC的保留抗张强度大于23MPa,断裂伸长率大于4%,裂解后试样的力学性能依然能够满足实际应用需要,因此PPC可以经受辐射消毒。     

聚合物辐射交联与裂解反应动力学

聚合物辐射交联和裂解的动力学分析结果表明,交联并不是严格地与剂量成正比。特别是在辐照初期很低剂量范围内,分子量异常地下降.辐照聚对苯二甲酸二醇酯的粘度测定支持了这一理论结果.     

磁场对聚合物立体构型影响的研究(Ⅰ)——聚甲基丙烯酸甲酯

本文研究了在甲基丙烯酸甲酯聚合过程中,磁场对产物中间同立构含量的影响。间同立构含量的测定是采用红外光谱定量法。实验结果表明: (1)聚甲基丙烯酸甲酯的间同立构百分含量S%值随磁场强度的增加按指数关系增加。 (2)聚甲基丙烯酸甲酯的玻璃化温度随磁场强度的增加而增加。 (3)聚甲基丙烯酸甲酯的平均分子量随磁场强度的增加,也按指数关系增加。 (4)通过公式计算了聚甲基丙烯酸甲酯分子链中能连续出现N个间同立构链节的组成几率F_N值。     

基底表面无规聚甲基丙烯酸甲酯立构复合结构的研究

采用原子力显微镜和反射吸收红外光谱研究了在基底上无规聚甲基丙烯酸甲酯立构复合结构的形成和结构特征,纯等规和间规聚甲基丙烯酸甲酯与等规/间规混合物(有立构复合结构生成)表面聚集形貌比较的结果表明,立构复合结构的生成使聚甲基丙烯酸甲酯在基底上形成树枝状的聚集形貌,因此无规聚甲基丙烯酸甲酯在基底上的树枝状聚集形貌表明了其内部生成了立构复合结构,而且这种结构对聚集形貌产生了重大影响,反射吸收红外光谱的研究表明,在基底表面薄膜中无规聚甲基丙烯酸甲酯主链结构比在本体厚膜中的更加伸展,更有利于立构复合结构的生成.     

预辐射聚丙烯反应挤出接枝丙烯酸的研究

利用电子束(EB)预辐照方法和反应挤出技术制备了聚丙烯接枝丙烯酸共聚物PP-g-AA. 采用化学滴定、红外光谱、偏光显微镜(PLM)、DSC和广角X射线衍射(WAXD)对接枝产物进行了表征. 研究结果表明, 接枝率随辐照剂量增加而增大并逐渐达到平台值, 但随单体浓度增大而表现为线性增加, 接枝链能起到异相成核作用, 从而提高了结晶速率并细化了球晶. 同时, 熔体流动速率(MFR)和力学性能测试结果表明, 预辐射和挤出过程造成了PP严重降解, 据此可认为接枝反应主要发生在聚丙烯断裂分子链的末端.     

聚异丁烯辐射裂解历程

1.研究聚异丁烯的辐射效应时,发现其裂解速度与温度关系与聚乙烯类似.这说明聚异丁烯在辐照时,除了直接因受射线作用而断链外,还可能同时进行一种由辐照时形成的自由基参加的二级反应. 2.在射线作用下形成的氢原子(由侧链CH_3-基的C-H键中断而产生),能与邻近的聚异丁烯分子的侧键CH_3-作用.由此形成的高分子自由基由于立体障碍不能起重合反应,但能起重排反应.其结果使双键产率与裂解产率的比值增加;使聚异丁烯的甲基侧链浓度下降而出现乙基支链. 3.??型高分子在溶胀状态下辐照,其裂解速度降低.这是因为当溶剂分子存在下抑制二分子重排裂解反应的缘故.共聚物??在含C~(14)甲苯中辐照后,引入高分子的放射活性随剂量增加而增加,但粘度不变.这也论证了上述假定是正确的. 4.研究了高分子量聚异丁烯级分与含C~(14)的低分子量聚异丁烯级分的混合物辐射效应.结果证明在辐照时,甲基从一聚异丁烯分子转移到另一分子上去.这结果说明聚异丁烯的辐射裂解过程,不仅是由于直接辐射效应的结果,而且还以二分子历程进行.     

X-ray and NMR measurements on irradiated polytetrafluoroethylene and polychlorotrifluoroethylene

The effects of ⁶⁰Co γ-radiation on polytetrafluoroethylene (PTFE) and polychlorotri-fluoroethylene (PCTFE) have been studied for radiation doses up to 940 Mrad. The dependence of per cent crystallinity upon irradiation level has been determined from x-ray analysis. An initial increase in crystallinity in PTFE, attributable to chain scission in the amorphous phase of the material, was found, followed (above 300 Mrad) by a gradual decrease associated with a disordering of the crystallites. No initial increase was observed for annealed samples of PCTFE due to the large initial value of the per cent crystallinity. Above 200 Mrad the crystallinity was found to decrease with accumulated dose. Nuclear magnetic resonance measurements on PTFE have indicated a radiation-induced broadening of the amorphous component of the NMR line appearing to maximize above 700 Mrad. Similar measurements of PCTFE have shown a narrowing of the crystalline component of the NMR line and subsequent appearance of the amorphous component at approximately 200 Mrad. The data indicate that the radiation-induced behavior of PTFE and PCTFE is similar above 200 Mrad.     

γ辐照 聚全氟乙丙烯(F46)的电子自旋共振研究 I.真空中俘获自由基的定量研究

A method for determining respectively the concentration of free radicials...CF2-CF2.(RI), ...CF2-CF-CF2...(RII)and...CF2- C(CF3)-CF2...(RIII) trapped in γ-irradiated F46 in vacuum at room temperature by analysing the ESR overlapping spectra is proposed. A quantitative relation between the concentration of free readicals and the total dose of γ-irradiation has been studied. The generating rate o free radicals caused by irradiation, i.e. G-value, has been calculated; it is 2.0 for RIII, 1.2 for RI, and 0.59 for RII. the magnitude of G value of free radicals is in the reverse order of their stability. Hence, we assume that the G value of free radicals in F46 mainly depends on the escaping rate of F2 and other fluorine-containing small molecules from surface of polymer into space. Therefore the looser the molecular chain, the larger becomes the G value of free radical. From that, we consider that both unstable free radicals RIII and RI with larger G-value mainly locate in the amorphous region, and the stable free radical RII with lower G-value is in the crystalline region. Recombinations between free radicals RII and RIII, or between RII and RI are forbidden at the temperature lower than 80C. An explanation for the saturation phenomenon of concentration of free radicals is given.     

Hydrolysis of post-consume poly(ethylene terephthalate) with sulfuric acid and product characterization by WAXD, C NMR and DSC

Post-consume PET was hydrolysed with commercial sulfuric acid (96%) with varying reaction times (5-120 min). The structure of the material obtained was analysed by ¹³C NMR, DSC, and WAXD and the results were correlated with reaction time. ¹³C NMR shows a decrease in chain size with reaction time and an increase in the number of carboxyl groups at the end of the chains. The correlation of DSC and WAXD data indicates the presence of structures of different sizes and an increase in crystallinity with reaction time. The structure of the samples hydrolysed for 5-60 min is less ordered than those of the samples hydrolysed for 60-120 min because the amorphous phase is predominantly quickly dissolved. Dissolution of the crystalline phase is favoured by the increase in reaction time. In this process, the crystalline memory retained in the dissolution of the crystalline phase behaves as nucleation sites which form smaller and more ordered structures compared to those obtained with shorter reaction times.     

Microstructural investigation of high‐speed melt‐spun nylon 6 fibers produced with variable spinning speeds

The structural details of high‐speed melt‐spun nylon 6 fibers at spinning speeds ranging from 4500 to 6100 m/min were investigated by solid‐state proton nuclear magnetic resonance (¹H NMR) spectroscopy, density and birefringence measurements, differential scanning calorimetry (DSC), and X‐ray diffraction (XRD). The analyses of the proton spin‐lattice relaxation times in the rotating frame and correlation times confirmed the existence of three different phases, the immobile crystalline, intermediate rigid amorphous, and mobile amorphous regions, in the fiber sample. At spinning speeds lower than 5200 m/min, the portion of the crystalline phase increased at the expense of the rigid amorphous region and then reached a plateau afterward, from which the mobile amorphous portion increased. Combined analyses of density and birefringence measurements, DSC, and XRD in conjunction with NMR results indicated that the formation of the γ crystal became predominant compared to that of the α crystal. The orientation factor of the crystalline phase increased slightly with increasing spinning speed, whereas the amorphous orientation factor decreased because of the increase of the purely amorphous region. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 1285–1293, 2000     

Dual lithium insertion and conversion mechanisms in a titanium-based mixed-anion nanocomposite

The electrochemical reaction of lithium with a vacancy-containing titanium hydroxyfluoride was studied. On the basis of pair distribution function analysis, NMR, and X-ray photoelectron spectroscopy, we propose that the material undergoes partitioning upon initial discharge to form a nanostructured composite containing crystalline Li(x)TiO(2), surrounded by a Ti(0) and LiF layer. The Ti(0) is reoxidized upon reversible charging to an amorphous TiF(3) phase via a conversion reaction. The crystalline Li(x)TiO(2) is involved in an insertion reaction. The resulting composite electrode, Ti(0)-LiF/Li(x)TiO(2) ? TiF(3)/ Li(y)TiO(2), allows reaction of more than one Li per Ti, providing a route to higher capacities while improving the energy efficiency compared to pure conversion chemistries.     

Small Pd nanoparticles supported in large pores of mesocellular foam: an excellent catalyst for racemization of amines

Highly dispersed palladium nanoparticles (1–2 nm) supported in large‐pore mesocellular foam (MCF; 29 nm) were synthesized. The Pd‐nanocatalyst/MCF system was characterized by transmission electron microscopy (TEM), powder X‐ray diffraction (XRD) and X‐ray photoelectron spectroscopy (XPS). The performance of the Pd nanocatalyst obtained was examined for amine racemization. The Pd nanocatalyst showed higher activity and selectivity toward racemization of (S)‐1‐phenylethyl amine than any other amine racemization catalyst reported so far and it could be reused several times. Our data from TEM and XRD suggest a restructuring of the Pd nanocatalyst from amorphous to crystalline and an increase in Pd nanocatalyst size during the racemization reaction. This led to an unexpected increase of activity after the first use. The Pd nanocatalyst obtained can be integrated with other resolving processes of racemic organic compounds to increase the yield of chiral organic products.     

Plastic deformation of poly(tetramethylene oxide). II. Molecular orientation as measured by x-ray diffraction and NMR measurements

The orientation of the crystalline and amorphous phases in uniaxially drawn samples of polytetramethylene oxide has been studied by x-ray and NMR methods. Pole figure measurements give the orientation of the crystalline phase. Its dependence on the draw ratio does not obey the pseudoaffine model. The crystalline fraction is derived from NMR measurements at temperatures between T_g and T_m, where the free induction decay (FID) of the unoriented sample can be analyzed in terms of a rigid (crystalline), a constrained, and an amorphous phase. Low temperature (T < T_g) measurements of the NMR second-moment anisotropy in protonated and deuterated samples give a mean orientation of the chains higher than that corresponding to the crystalline phase. The lack of anisotropy in the tail of the FID at temperatures between T_g and T_m indicates no appreciable anisotropy in the truly amorphous interlamellar phase. From this and from the ratio of the P₄/P₂ orientations, factors which obey the “most probable distribution,” it is concluded that the amorphous orientation is due to the layer of constrained chains at the surface of the lamellae.