用等离子体增强化学气相沉积技术制备类金刚石碳薄膜的摩擦磨损性能研究

利用射频-直流等离子体增强化学气相沉积技术在单晶硅衬底上沉积类金刚石碳薄膜,采用激光拉曼光谱仪和原子力显微镜对薄膜的结构和表面形貌进行表征,采用纳米压痕仪测定薄膜的硬度,并用UMT型微摩擦磨损试验机考察了薄膜在不同试验条件下的摩擦磨损性能.结果表明:所制备的类金刚石碳薄膜表面光滑致密且硬度较高;在干摩擦条件下与GCr15钢球或Al2O3球配副时显示出良好的减摩抗磨性能,摩擦系数较低,耐磨寿命较长,而在水润滑条件下同Al2O3球配副时发生灾难性磨损.     

一种氯苯基硅油的合成及其摩擦磨损性能研究

合成了一种甲基封端、侧基含五氯苯基取代基团的有机聚硅氧烷(CPSO),考察了CPSO的粘温性能、倾点、饱和蒸气压及热稳定性能.采用OptimolSRV型微动摩擦磨损试验机评价了CPSO及空间用润滑油全氟聚醚(PFPE)和磷嗪(X-1P)在常温常压下用于GCr15/CuSn合金摩擦副润滑剂的摩擦磨损性能;采用CZM型真空摩擦试验机评价了3种润滑油在真空条件下用于GCr15/CuSn合金和GCr15/9Cr18摩擦副润滑剂的摩擦磨损性能.结果表明:在真空和常温常压条件下,CPSO的减摩和抗磨损性能均优于PFPE及X-1P;与此同时,CPSO具有极低的饱和蒸气压、很低的热挥发损失以及较好的热稳定性和低温流动性.故其在空间飞行器械运动部件润滑领域具有广泛的应用前景.     

一种可反应性纳米SiO2的制备和表征及其摩擦磨损性能研究

以正硅酸四乙酯为前驱体,以含不饱和双键碳链为修饰剂采用原位表面修饰法合成出1种可反应性纳米二氧化硅并对其结构进行表征;测定其透光率并得出在介质中的分散性;采用往复摩擦磨损试验机和四球摩擦磨损试验机考察纳米二氧化硅作为汽油机油添加剂的摩擦磨损行为,并用扫描电子显微镜及能量色散谱仪对其磨痕进行观察和分析.结果表明:SiO2 纳米微粒可以直接分散于基础油等油性介质中并具有良好的分散稳定性;作为润滑油添加剂表现出优异的抗磨减摩性能,并对磨损表面起到一定的修复作用.这是由于含双键有机物的存在,在摩擦过程中形成了聚合物膜而起到良好的减摩作用.     

火焰喷涂聚苯硫醚(PPS)复合涂层在水环境中的摩擦磨损性能研究

利用火焰喷涂技术在45#钢表面制备了炭纤维增强聚苯硫醚复合涂层并研究了其结构和力学性能,采用MM-200型摩擦磨损试验机对比考察了复合涂层同不锈钢对摩时在干摩擦与水环境中的摩擦磨损性能,并对涂层及偶件磨损表面形貌进行观察分析,采用X射线光电子能谱仪分析了偶件磨损表面典型元素的化学状态,探讨了涂层在水环境中的抗磨机理.结果表明:用火焰喷涂工艺制备聚苯硫醚复合涂层的过程中,聚苯硫醚粉末未发生明显降解与氧化;炭纤维含量影响复合涂层的粗糙度、显微硬度及与底材的结合强度;在水环境中炭纤维增强聚苯硫醚涂层表现出比聚苯硫醚涂层更优良的抗磨性能,这是由于水的冷却与冲刷作用使得复合涂层向偶件磨损表面的粘着转移明显减轻的缘故.     

二硫化钼改性热塑性聚酰亚胺复合材料的摩擦磨损性能研究

采用热压成型工艺制备MoS2 填充热塑性聚酰亚胺复合材料,测定了其弯曲强度和压缩强度,采用MPX-2000型摩擦磨损试验机评价MoS2 填充热塑性聚酰亚胺复合材料在干摩擦和水润滑2种工况下的摩擦磨损性能,利用扫描电子显微镜观察和分析材料磨损表面形貌和元素分布.结果表明:与聚酰亚胺树脂相比,加入MoS2后复合材料的弯曲强度和压缩强度有所降低,随着MoS2含量增加,材料的弯曲强度和压缩强度趋于稳定;在干摩擦条件下,MoS2逐步在磨损表面富集,相应的摩擦系数有所降低;MoS2含量为10%时磨损表面仅出现局部熔融,磨损率最低,当MoS2含量为20%时磨损表面出现深度熔融,磨损率较大;在水润滑条件下,MoS2仍起到良好的润滑作用,摩损率较干摩擦条件下降低1个数量级,表现出疲劳磨损特征.     

基于改进无迹卡尔曼滤波器算法的滞回模型参数识别研究

地震产生的周期荷载作用下,钢混桥墩结构表现出滞回行为。为描述滞回行为,研究者提出各类滞回模型,其中BWBN(Bouc-Wen-Baber-Noori)模型可以描述结构滞回行为的强度退化、刚度退化和捏拢效应等典型特征。此外,无迹卡尔曼滤波器UKF(unscented Kalman filter)算法是识别BWBN模型参数的高效方法,但当参数初始值与真实值的偏差过大及缺乏对系统的整体估计时,UKF算法识别过程受到局限。本文改进生成样本点规则,提出改进UKF算法。数值模拟结果表明,在无噪声条件下,改进UKF算法识别得到的参数估计值与准确值的误差平均为1.51%,最大误差为4%;在2%均方根RMS(root mean square)高斯白噪声条件下,误差平均为5.43%,最大误差为18%;在5%RMS高斯白噪声条件下,误差平均为8.9%,最大误差为26%和22%。改进UKF算法识别非线性滞回系统状态估计和BWBN模型参数更加准确和稳定。     

Effect of the liquid–liquid phase separation on the crystallization behavior of a poly(ethylene‐ran‐vinyl acetate) and paraffin wax blend

The effect of liquid–liquid phase separation (LLPS) on the crystallization behavior of poly(ethylene‐ran‐vinyl acetate) with a vinyl acetate content of 9.5 wt % (EVA‐H) in the critical composition of a 35/65 (wt/wt) EVA‐H/paraffin wax blend was investigated by small‐angle light and X‐ray scattering methods and rheometry. This blend exhibited an upper critical solution temperature (UCST) of 98°C, and an LLPS was observed between the UCST and the melting point of 88°C for the EVA‐H in the blend. As the duration time in the LLPS region increased before crystallization at 65°C, both the spherulite size and the crystallization rate of the EVA‐H increased, but the degree of the lamellar ordering in the spherulite and the degree of crystallinity of the EVA‐H in the blend decreased. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 707–715, 2000     

Crystallization kinetics of poly(trimethylene terephthalate)

The isothermal crystallization kinetics of poly(trimethylene terephthalate) (PTT) have been investigated using differential scanning calorimetry (DSC) and polarized light microscopy (PLM). Enthalpy data of exotherm from isothermal crystallization were analyzed using the Avrami theory. The average value of the Avrami exponent, n, is about 2.8. From the melt, PTT crystallizes according to a spherulite morphology. The spherulite growth rate and the overall crystallization rate depend on crystallization temperature. The increase in the spherulitic radius was examined by polarized light microscopy. Using values of transport parameters common to many polymers (U* = 1500 cal/mol, T_∞= T_g − 30 °C) together with experimentally determined values of T (248 °C) and T_g (44 °C), the nucleation parameter, k_g, for PTT was determined. On the basis of secondary nucleation analyses, a transition between regimes III and II was found in the vicinity of 194 °C (ΔT ≅ 54 K). The ratio of k_g of these two regimes is 2.1, which is very close to 2.0 as predicted by the Lauritzen–Hoffman theory. The lateral surface‐free energy, σ = 10.89 erg/cm² and the fold surface‐free energy, σ_e = 56.64 erg/cm² were determined. The latter leads to a work of chain‐folding, q = 4.80 kcal/mol folds, which is comparable to PET and PBT previously reported. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 934–941, 2000     

On the Eigenvalues of Half‐Linear Boundary Value Problems

We consider the half‐linear boundary value problem where and the weight function q is assumed to change sign. We prove the existence of two sequences , of eigenvalues and derive asymptotic estimates for as .     

Solubility of vinylidene fluoride polymers in supercritical CO2 and halogenated solvents

The cloud‐point behaviors of poly(vinylidene fluoride) (PVDF) and poly(vinylidene fluoride‐co‐22 mol % hexafluoropropylene) (VDF–HFP₂₂) are reported at temperatures up to 250 °C and pressures up to 3000 bar in supercritical CO₂, CHF₃, CH₂F₂, CHClF₂, CClF₃, CH₃CHF₂, CH₂FCF₃, CHF₂CF₃, and CH₃CClF₂. The molecular weight of PVDF has a smaller effect on the cloud point than the solvent quality. Cloud‐point pressures for both fluoropolymers decrease as the solvent polarizability, polar moment per molar volume, and density increases. However, it is extremely difficult to dissolve either fluoropolymer in CClF₃, which has a large polarizability and a small dipole moment. CO₂ is an effective solvent because it complexes with the C F dipole at low temperatures where energetic interactions fix the phase behavior. In addition, polymer architecture has a strong impact on the cloud‐point pressure. VDF–HFP₂₂ has lower cloud‐point pressures than PVDF in all solvents because it has a larger free volume that promotes facile interactions between the solvent and the polymer segments. Cloud‐point data are also reported for amorphous poly(tetrafluoroethylene‐co‐x mol % 2,2‐bistrifluoromethyl‐4,5‐difluoro‐1,3‐dioxole) (TFE–PDD_x ; x = 65 and 85) in CO₂. These data provide an interesting comparison to the PVDF–CO₂ and VDF–HFP₂₂–CO₂ systems because TFE–PDD₆₅ and TFE–PDD₈₇ have very high glass‐transition temperatures of 160 and 240 °C, respectively. © 2000 John Wiley & Sons, Inc. J Polym Sci B: Polym Phys 38: 2832–2840, 2000