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71.
《国际聚合物材料杂志》2012,61(1-2):51-70
Abstract Poly(ether ester)s (PEE) based on poly(butylene terephthalate) (PBT) as hard segments and poly(ethylene glycols) (PEG) with different molecular weight as soft segments are studied by means of WAXS and SAXS in the drawn and undrawn state after annealing at various temperatures (Ta ). The repeatedly reported strong increase of the long spacing L with Ta is confirmed once again. In the same time the directly measured by WAXS crystallite size of PBT remains insensitive to Ta and the increase of L with Ta is the stronger, the higher the PEG content. It is concluded therefore that the rise in L is due to the expansion of the amorphous intercrystalline layers rather than to crystal thickening, the latter being the case of semicrystalline homopolymers. The observed much stronger increase of L with Ta in undrawn samples than in drawn ones is explained by melting of less perfect crystallites at higher Ta and dephasing processes in the amorphous regions. The conclusions drawn seem to be valid for other segmented polyblock copolymers and suggest some specific features of the block copolymers in comparison to homopolymers. 相似文献
72.
金属锂具有极高的理论能量密度,是新一代锂电池中最有潜力的负极材料之一。金属锂沉积时容易形成枝晶,极大影响了锂金属电池的安全性与使用寿命。但由于金属锂性质活泼,缺乏锂电极/电解液界面原位表征方法,锂枝晶生长机制尚不明确。通过有限元方法,基于非线性电极过程动力学,以三次电流模型定量研究了电极/电解液界面行为,并分析不同过程参数对表面电流的影响。结果表明,电极/电解质界面的浓度、电场差异是枝晶生长的主要原因,更大的扩散系数有利于提高界面浓度均匀性,更小的交换电流密度有利于减弱界面反应的敏感性。存在电化学极化区间是均匀沉积的必要条件,电化学极化区间越宽,均匀沉积操作窗口越宽。通过极化曲线可以判断体系是否具有均匀沉积的倾向。加深了对锂电极/电解液界面的电沉积过程的理解,对锂负极保护研究具有指导性意义。 相似文献
73.
以某建筑场地边坡的实际地质条件为基础,建立了边坡稳定性的FLAC 3D数值模拟模型,分别分析了有无支护3种工况下的边坡稳定性,研究了边坡安全稳定系数随抗滑桩加固位置、长度和桩间距的变化规律,给出了合理的抗滑桩设计方法。结果表明:(1)边坡的最大水平位移和竖向位移出现在素填土层的坡顶和坡中位置,无支护条件下难以满足安全储备要求;(2)合理的抗滑桩加固位置可以将边坡安全稳定系数提高到满足安全储备要求,抗滑桩的最佳加固位置为边坡中部距底坡水平距离为34m处;(3)边坡的安全稳定系数随抗滑桩长度的增大和桩间距的减小而增大,抗滑桩的最佳长度和间距分别为20m和8m。 相似文献
74.
王守鹏 《吉林化工学院学报》2022,39(7):6-11
根据电力巡检需求,提出以可调五杆机构为基础的弹性越障巡检机器人的设计方案.设计的主要内容包括:电力巡检可调机器人三维数字化建模,运动仿真、静载荷分析、结构优化分析、越障机构设计,并用UG运动学仿真模块对防振锤越障进行运动仿真,验证方案的可行性. 相似文献
75.
J. Ruud van Ommen John van der Schaaf Berend G.M. van Wachem Cor M. van den Bleek 《Powder Technology》2004,139(3):264-276
Pressure data sampled at sufficiently high frequency (typically 20 Hz or higher) can yield much information about the hydrodynamic state of a fluidized bed. Since part of the pressure waves travelling through large (industrial) fluidized beds is only detectable in a limited area of the bed, pressure measurements need to be performed at several positions to cover the whole bed. We examine these local pressure waves (caused by, e.g., passing bubbles or coalescing bubbles) in a 0.80 m i.d. bubbling fluidized bed of Geldart B particles. Experiments and simulations are performed to determine the intensity decrease as local pressure waves propagate from their origin. A new spectral method is applied to determine the degree of coherence for pressure signals measured at two different positions in a fluidized bed. For a superficial gas velocity of 5umf, local pressure waves can be detected up to a radial distance of about 0.5 m from their origin; this distance is somewhat lower for lower gas velocities. This means that the radial spacing of pressure probes should not exceed 1 m. For large diameter beds with a bed height below 1.5 m, a set of probes at a single level and at several radial positions is sufficient to observe or monitor the dynamic state of the complete bed; the probes should preferably be placed at a height of 30% to 40% of the total bed height. 相似文献
76.
When fibrillation occurs during peeling, the normal stress in the adhesive may gradually reduce to zero at the peel front. The shear stress also reduces to zero. Classical beam-spring (or beam-on-elastic-foundation) models do not yield solutions that have these properties. With the use of a beam-on-foundation model combined with a cohesive zone in the neighborhood of the peel front, these properties can be satisfied. In order to obtain analytical solutions, peel tests are considered in which the backing has a small slope and is linearly elastic in the adhered region, and the traction law is assumed to be piecewise linear. Cases are considered with only normal stresses in the adhesive (mode I), only shear stresses (mode II), and both stresses coupled (mixed-mode behavior). Analytical solutions are obtained for displacements of the backing, forces in the backing, and stresses between the adhesive and the backing. 相似文献
77.
A mandrel peel test is established for measuring the adhesive fracture toughness of a metal/rubber-toughened epoxy laminate system. By adopting an energy balance analysis it is possible to determine directly both adhesive fracture toughness and plastic work in bending the peel arm around the mandrel. The suitability of the procedure is examined for various types of metal peel arms, which are classified in terms of their ability to deform plastically during the test. The plastic work is also predicted theoretically, and comparisons are made between the measured and calculated values. The fracture energies determined from the mandrel tests are compared with those obtained from 90° fixed-arm peel tests. For the calculations of plastic work in bending in the fixed arm test, various options are used when modelling the tensile stress-strain behaviour of the peel arm material. In addition, the adhesive layer thickness is considered in terms of its influence on the calculation of adhesive fracture toughness. 相似文献
78.
以高岭石-甲醇(K-M)复合物为前驱体,利用置换法于常温下制备了3种高岭石-氨基硅烷插层复合物。用X射线衍射、Fourier变换红外光谱仪、透射电子显微镜、热分析仪等对复合物进行了表征。结果表明:3种高岭石-氨基硅烷插层复合物的层间距均扩大至2nm以上,插层率都大于95%。3种氨基硅烷分子均和K-M前驱体的甲氧基共同存在于高岭石层间,均呈两层倾斜排列,倾斜程度不同。氨基硅烷的插入破坏了高岭石层间的氢键,加剧了高岭石自身结构中硅氧四面体片层与铝氧八面体片层之间的错位,使得复合物片层出现不同程度的卷曲变形。3种高岭石-氨基硅烷插层复合物的热分解过程均分三步进行:表面水的蒸发及层间甲氧基的脱嵌分解、插层剂氨基硅烷分子的脱嵌、高岭石脱羟基。 相似文献
79.
为了探究三角翼涡流发生器的纳米氧化镁颗粒污垢特性, 选用粒径为50 nm的氧化镁颗粒配制的胶体溶液为研究对象, 研究了在不同水浴温度、颗粒浓度、流速、三角翼间距以及不同布置等工况下三角翼涡流发生器的污垢特性。结果表明:三角翼涡流发生器具有抑垢特性, 水浴温度、浓度、流速对其抑垢能力及结垢速率均有影响, 水浴温度升高、颗粒浓度降低以及工质流速升高都会导致三角翼的抑垢能力增强。三角翼不同列间距的抑垢能力随着布置方式的改变而改变, 采用均匀分布布置形式时40 mm列间距的抑垢能力最强, 而采用同列数布置时80 mm列间距的抑垢能力最强。 相似文献
80.
以丙烯酰胺(AM)和溴化N-烯丙基吡啶([APy]Br)为单体,制备了一种离子液体聚合物黏土抑制剂AM/[APy]Br。通过单因素实验法确定了最佳反应条件为:m(AM)∶m([APy]Br)=15∶1,w(引发剂)=0.8%,其中,n(K2S2O8)∶n(Na HSO3)=1∶1,反应温度50℃。并对AM/[APy]Br进行了FTIR和1HNMR表征,对其性能进行了评价。结果表明,在室温下,2 000 mg/L AM/[APy]Br溶液防膨率为80.90%,当温度为90℃时,其防膨率仍达77.97%;2 000 mg/L AM/[APy]Br溶液与0.3 mol/L KCl溶液复配后,防膨率可达96.20%;与0.2 mol/L KCl溶液复配后,防膨率高于0.3 mol/L KCl溶液,复配溶液经4次冲刷,防膨率仍可达76.17%;占溶液总质量3.0%AM/[APy]Br与3.0%KCl复配溶液浸泡后的Na-MMT晶层间距(1.57 nm)明显优于单独使用同等浓度KCl浸泡后的Na-MMT晶层间距(1.62 nm)。 相似文献