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在浓硫酸或稀硫酸中聚合得到了高分子量P2VP,~(13)C-NMR谱确定其为无规聚合物。特性粘数(切变速度D=0)与分子量之间的关系为[η]_(D=0)=1.27×10~(-2)(?)_W~(0.70)(在DMF中,25℃,(?)_W=2.66×10~6—10.0×10~6)。在DMF中,25℃,不依赖于切变速度的最大特性粘数为260毫升·克~(-1),相应的分子量M_η=1.74×10~6左右。无扰尺寸(_0/M)=6.08×10~(-18)厘米~2·克~(-1),在DMF 中B参数为1.91×10~(-27)厘米~3。 相似文献
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在不同外加水压下作者等用毛细管粘度计测定了聚甲基丙烯酸甲酯五个分级试样的苯溶液粘度,并用光散射法在丙酮溶液中测定了重均分子量,得到下列特性粘数、分子量关系式(25°)。不加外压时:[η]=3.80×10~(-3)M~(0.79)毫升/克S_R=55达因/厘米~2:[η]_s=12.6×10~(-3)M~(0.70)D_R=5000秒~(-1):[η]_D=8.37×10~(-3)M~(0.73) 适用于分子量范围0.2—4.5×10~6。并指出用实验数据验证性粘数理论时,α值的切变速度依赖性有重要的影响。粘度数据中斜度系数 k′或β值,无论对 S_R 或 D_R 都没有显著的影响,与前人的结果有不同。对光散射测定所用仪器加以叙述并从光散射数据得到了试样的 A_2和<~2>_z 的数值。 相似文献
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对聚二甲基硅氧烷-溴代环己烷θ溶液(28℃)体系进行了沉降速度法测定分子量分布及沉降系数压力改正的研究。提出了一种新的直接测定沉降系数的压力改正的方法,即在沉降池中加入不同量的溶液以得到不同的液柱高来改变静压,测定溶液界面在不同静压下的浮升速度计算压力系数。所得适用 于静压为200大气压以下的沉降系数的压力改正系数α=1.44×10~(-3)_(大气压)~(-1)。从沉降系数分布、(?)_ω、[η]_θ及[η]_(甲苯)的测定,订定了聚二甲基硅氧烷在28℃θ条件下的s-M,[η]_θ-M及在甲苯(25℃,良溶剂)中的[η]-M单分散关系为。 s_1=6.30×10~(16)M~(0.50)(溴代环己烷,28℃) [η]=7.41×10~(-2)M~(0.50)(溴代环己烷,28℃) [η]=9.53×10~(-3)M~(0.71)(甲苯,25℃) 相似文献
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SiO2负载的后过渡金属配合物/三乙基铝催化乙烯聚合研究 总被引:5,自引:0,他引:5
将后过渡金属配合物{[2,6-ArN=C(Me)2C5H3N]FeCl2} ( Ar=2,6-iPr2C6H3) Ⅰ负载于SiO2上, 并与三乙基铝(AlEt3)组成催化剂体系并催化乙烯聚合. 考察了Al/Fe比(AlEt3/催化剂摩尔比)、聚合温度对催化剂活性、聚乙烯(PE)分子量、熔融温度以及结晶度的影响. 在Al/Fe比为750、聚合温度为40 ℃时, 催化剂活性达到7.07×105g PE·(mol Fe·h)-1. 实验所得聚合物的分子量为1.05×105~2.33×105 g/mol, 熔融温度高达132 ℃左右,结晶度在44.2%~77.8%之间. 相似文献
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对低温聚合丁苯橡膠一个级分(M=1.0×10~6)的甲苯溶液在切变速度 D=10—20,000秒~(-1)范国内测定了五种浓度溶液的粘度数据(25.0℃)。粘度计采用 Tsuda 的水平毛细管水平流出体积计量管的设计,且在全部切变速度范围内都从同一毛细管流出,使不同范围内的数据很好衔接。实验结果证明在低切变速度区域牛顿粘度η(?)(0)的存在。并且从lnη(?)—ln D 曲线的反曲点(?)值不依赖于浓度和对反曲点的对称性估计η(?)(∞)值和整个切变速度范国内的粘度行为。取几个等 D 值时的 lnη(?)按(lnη(?)/C)-C 的线性外推得到[η]_D,明确表示在低切变速度区域[η](?)的存在。两种牛顿流动间转变区域的实难数据可以采用下列两公式线性化:x(D)=(1/2)[1-erf(kln(?))],x(D)=(1/1+(?))~n,式中x=(lnη(?)-lnη(?)(∞)/lnη(?)(0)-lnη(?)(∞)),erf(z)=(?)-u~2du,k 和 n 是依赖于浓度的参数,但在较高浓度时均趋向一恒定值。([η]_D/[η]_0)-ln D 曲线相当符合于刚性橢球轴比 p=4—5间的理论曲线,这样得到的转动扩散系数(?)_(rot)=6.6×10~2秒~(-1),但是从(?)_(rot)和[η]_0值按 Scheraga-Mandelkern 方法计算得到的分子量值与实际不符,所以丁苯橡膠分子线团不是刚性结构;而以1/(?)值作为高分子线团弹性变形的松弛时间,按 Bueche 理论计算得到的分子量值与实际极相一致。 相似文献
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本文用GPC结合特性粘度的方法,对聚辛烯-1四氢呋喃体系的Mark-Houmink常数进行订定。数据处理采用了Weiss法和流体力学平均分子量(?)_x两种方法,α值分别为0.701和0.625,相对误差10%左右,所得Mark-Hon-Wink方程Weiss法为:[η]_(THF)~(25℃)=3.89×10~(-4)[M]~(0.701)(?)_x法为[η]_(THF)~(℃25)=4.14×10~(-4)M~(0'625)。本文还研完了聚合反应条件对聚辛烯-1分子量及分子量分布的影响。发现三种TiCl_3为主催化剂,三乙基铝为助催化剂时,其GPC谱图均为双峰型,两个峰的比例随聚合反应条件不同而变化。表明聚合体系至少有两种不同性质的活性中心,有着不同的形成和增长速率。 相似文献
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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
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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
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不同分子量尼龙1010的结晶与熔融*朱诚身王经武王友文杨桂萍(郑州大学材料工程系郑州450052)陈玉莫志深(东北师范大学分析测试中心长春130024)(中国科学院长春应用化学研究所长春130022)关键词尼龙1010,分子量,结晶,熔融*1994_... 相似文献
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QIAN Baogong 《高分子科学》1988,(2):97-116
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
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In this paper,crystallization kinetics of a series of ethylene-propylene copolymers prepared by living polymerization coordination catalyzed by a fluorinated bis(phenoxyimine)Ti catalyst(FI-EP copolymers)was studied,and was compared with that of ethylene-propylene copolymers prepared by a conventional Ziegler-Natta catalyst(ZN-EP copolymers).It is found that,the Avrami exponent and the crystallization rate constant of the FI-EP and ZN-EP copolymer show similar dependence on crystallization temperature,bu... 相似文献