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1.
本文用广角X-射线衍射法(WAXD)研究了稀土催化聚合顺-1,4-聚丁二烯(Ln-PB)低温下分子量和温度对结晶过程的影响.随着分子量的改变,结晶速度在M_η=8×10~5左右有一极小值;在M_η=29×10~5左右有一极大值.最大结晶速度发生在T_(c,max)=-60~-70℃之间.最大平衡结晶度值,在M_η大于10~6以上与分子量无关,而最大平衡结晶度值所对应的温度与M_η呈线性关系.随着温度上升,晶胞参数略有增大.Ln-PB主级结晶属于非均相成核,以原纤状和盘状混合生长.  相似文献   

2.
徐洋 《应用化学》1986,(5):38-38
以稀土催化剂聚合得到的聚丁二烯(Ln-PB)的顺式含量接近99%,支化度小,分子具有较高的规整性。本工作用电镜,线膨胀仪、体膨胀仪、DSC、GPC、X-光衍射等实验方法在较宽的分子量范围和结晶温度范围下对Ln-PB的本体结晶和溶液结晶行为进行了研究。  相似文献   

3.
本工作以线膨胀、体膨胀、DSC、扭辫等方法,在较宽的分子量和结晶温度范围内研究了稀土顺-1,4-聚丁二烯(Ln-PB)的分子量与结晶速率,结晶熔点,玻璃化温度及结晶比表面能之间的关系。进一步考察了分子链缠结对结晶速率的影响,并在结晶成核理论的基础上引入链缠结的影响,导出Ln-PB的结晶动力学方程,得到了与实验符合较好的结果。  相似文献   

4.
本工作用WAXD法对以环烷酸稀土盐为主的催化剂合成的丁二烯和异戊二烯共聚物(Ln-PBI)在低温下的结晶行为进行了研究。Ln-PBI室温下为非晶态,在低温下,异戊二烯含量(重量)>20%时不能生成结晶;含量(重量)<20%时,可观察到结晶的生成。并且结晶度随结晶温度的下降而增加,晶格常数则逐渐减小。Ln-PBI基本上保持了Ln-PB单斜晶系的结晶结构,其晶区由Ln-PB链段所贡献。  相似文献   

5.
利用相转换法制备了聚酰亚胺吸附萃取搅拌棒,用5种有机酚作为评价标样,并与现有商品化吸附萃取搅拌棒进行比较。优化了萃取搅拌速度、溶液离子强度、萃取温度、萃取时间以及热解析温度和时间。在最佳实验条件下,100 mL 样品,30% NaCl,在25℃下,经活化5 min 后的聚酰亚胺吸附搅拌棒萃取30 min (800 r/ min),然后300℃热解析4 min,使目标物脱附,再进行色谱分析。目标物在大于两个数量级浓度范围内具有良好的线性(R≥0.9995),定量限(LOQ,S/ N=10)为0.028~0.123μg/ L,重复性为1.6%~9.7%。将SBSE 与气相色谱-质谱联用,对海水、自来水和污水中的酚类进行定性与定量分析,结果表明,聚酰亚胺吸附萃取搅拌棒具有良好的选择性,最高热解析温度350℃,在分析水中痕量极性化合物领域具有广阔应用前景。  相似文献   

6.
本文研究了镧系稀土元素催化聚合的顺-1,4-聚丁二烯(Ln-PB),其顺式含量不小于97%,最近测得达99.8%,比过渡元素(如Ti,Co,Ni等)催聚为高,并可与铀催聚的U-PB相比拟.对Ln-PB的表征,文中考察了它与Ni等经典催聚的异同,结果认为稀土催化聚合的高顺-1,4-聚丁二烯的大分子以线性良好,不易缠结为其分子结构特征,导致稀溶液性质、结晶行为、本体粘度、应力松弛、屈服强度等性能与支化的Ni-PB相区别。  相似文献   

7.
本工作研究了稀土催化聚合的聚丁二烯(Ln-PB)的结晶速率与分子量的关系。结果表明Ln-PB的结晶速率在η=5.6×105左右有一极小值,而在η=3.4×106左右有—极大值。 从实验中还发现,Ln-PB的结晶在-20℃左右,由单二维核生长逐渐转变为多二维核生长。 本作工根据结晶成核理论,计算了不同分子量Ln-PB结晶折叠面的比表面能,σe表明当 η<106时,σ3随分子量的变化很小;当η>106时,σe随分子量的增加明显增大。  相似文献   

8.
用玻璃外循环无梯度反应器研究在Pt/Al2O3催化剂上丁烷、反-2-丁烯及顺-2-丁烯深度氧化的内扩散影响.测出催化剂有效因子η为0.42~1.27,并随反应温度升高而下降.用Runge-Kutta法计算氧在催化剂孔内压力分布,孔中心氧分压y0随内扩散影响加大而下降,在420℃y0如趋于零.  相似文献   

9.
平板显示是显示技术发展的方向,发光材料的薄膜化是显示技术发展的重要研究对象.本研究采用电沉积-烧结方法制备出了氧化钇铕红色荧光薄膜.在0.1 mol/L硝酸钇溶液中加入4%(摩尔分数)0.1 mol/L硝酸铕掺杂,用三电极体系进行阴极电沉积,工作电极的电位为-1.2 V(相对于Ag/AgCl电极),温度65℃,沉积时间为400 s,500℃灼烧2 h,制备出的发光薄膜与高温固相法制备的薄膜对比,其发射光谱的峰位相同.XRD检测显示经不同温度灼烧后,随温度的升高,氧化钇晶相逐渐完整.经SEM扫描,薄膜沉积均匀平整.  相似文献   

10.
聚硫堇的电导率为9.6×10-6 S•cm-1,属有机半导体.在10 ℃至60 ℃温度范围内,测定了聚硫堇的循环伏安图、恒电位下的放电曲线和交流阻抗图,并测定了电解质溶液的电导率随温度的变化.在聚硫堇的循环伏安图上有一阳极峰和一阴极峰,它们的峰电流均随温度的升高而增加;恒电位下的放电电流也随温度升高而增加;而交流阻抗的结果表明,聚硫堇的电荷传递电阻Rct随温度升高而下降,即它的交换电流i0随温度升高而增加;而溶液电阻和膜电阻也随温度的升高而下降,这同样会引起电流随温度升高而增加.所以温度对固体半导体聚硫堇的电极反应速率的影响包含了电极反应的本身和电极的电导率等因素的影响.聚硫堇的扫描电镜图证实了它的表面是一种纤维状结构.  相似文献   

11.
In this work, the stirring induced solution crystallization behaviour of cis-1, 4-polybutadiene polymerized with rare-earth catalyst (Ln-PB) has been studied by electron microscope, DSC and GPC. It has been found that when 0.5% Ln-PB toluene solution was stirred at a temperature within the range of-15°to-79℃with a speed of 180 rpm, a kind of white swollen thread-llke substance wound around the stirrer was formed. It was seen under electron microscope that this swollen thread-Like substance consisted of fibrillar crystals of Ln-PB parallel to each other. The amount of Ln-PB wound around the stirrer increased with the decrease in crystallization temperature until a maximum was reached at about-65℃, then it decreased with the decrease in crystallization temperature. However, the higher the crystallization temperature, the higher the average molecular weight and the narrower the molecular weight distribution of Ln-PB which wound around the stirrer. Therefore, Ln-PB sample may be fractionated by stirring its dilute solution at a series of crystallization temperatures.  相似文献   

12.
The effects of molecular weight and temperature on crystallization processes at low tempera-ture for cis-1,4 polybutadiene prepared with rare-earth catalyst (Ln-PB) have been studied by WAXDmethod. In the range of molecular weight from  相似文献   

13.
本文用电镜研究了经过分级得到的不同分子量及不同分子量分布的稀土顺1,4 聚丁二烯(Ln-PB)及镍顺1,4 聚丁二烯(Ni-PB)的低温结晶形态、结晶成核及生长机理。发现低分子量 PB以预现成核为主,而高分子量PB以大分子的缠结为中心的散现成核为主,得到两种不同片层缠结形态的PB球晶。其结晶形态及速率主要受高分子量中的大分子缠结影响。  相似文献   

14.
For the mechanism of isothermal bulk crystallization of high polymers, beside the nucleation and growth steps, the unimpingement of growing crystal aggregates should be taken into account for the modification of the Avrami equation. Starting from Poisson distribution function of growing crystal aggregates, the probability of the unimpinging ones should be P(0)+P(1), then the Q-modified Avrami equation thus derived can be expressed aswhere V0 represents the volume fraction of crystal aggregates at crystallization time t at a given temperature, while the exponent n on t relates to the mode of nucleation and growth, and K_q is the corresponding shape factor. This Q-modified one is verified satisfactory by the isothermal bulk crystallization of lanthanidecatalytically polymerized polybutadiene (Ln-PB), polyisoprene (Ln-PIR) and their copolymers (LnPB/IR). Furthermore, the proposed mechanism is well identified by the change of morphological state during the course of crystallization of the corresponding east film of Ln-PB TR (92/8) at-60°(Fig. 1).Upon examination of the influence of the number of entanglement on crystallization rate, it reveals the existence of two stages of entanglementation, the primary and the secondary ones (Fig. 19)The equation for dependence of molecular weight and entanglement on bulk crystallization rate has been derived as Eq. 13 or 18 for Ln-PB, and verified by the experimental rate data of well fractionated Ln-PB samples crystallized at -9.1 to -15℃(Fig.20).  相似文献   

15.
The morphological structure and mechanism of nucleation and growth of Ln-PB and Ni-PBwith different molecular weight were investigated by transmission electron microscopy. The crys-tallization of low molecular weight fraction is primarily from predetermined nuclei, crystallizationfor the high molecular weight fraction is primarily from sporadic nuclei. Two types morphologyof spherulite with different lamellar entanglement have been observed. The entanglement of highermolecular weight fractions are found to be of significance in the morphology and rate of crystallizationof polymer.  相似文献   

16.
用小角光散射、电子显微镜等方法研究了熔体温度对熔融结晶的PTFE结晶形态的影响。结果表明,当熔体温度超过400℃时,PTFE的结晶形态从棒晶逐步向球晶转化,力学性能也随之变坏。DSC的研究阐明,形态与力学性能的变化是由于大分子的降解,而不是因为熔体中发生了物理转变所致。  相似文献   

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