聚合物中激化的冷冻和热刺激

用等速升温、阶路升温、剩余电荷等方法测量了聚丙烯的热刺激电流。对于α和β峰，冷冻电荷方法有更高的分辨率和对称的线型。热刺激电流包含了快极化和慢极化机构的贡献，但线型主要决定于后者。慢极化涉及聚合物长分子链局部链段的运动与束缚空间电荷的相互作用。     

有机液体的慢极化介电谱

高绝缘液体存在一种特殊类型的极化响应; 其性质很不同于普通的介电极化响应。后者可用频域方法描述, 称为快响应;前者不能用频域而只能用时域方法描述, 故区别地称为慢响应。在微分时域介电谱中, 每种快或慢极化机构贡献一个峰。苯的时域谱有一个快峰和两个慢峰。室温下石蜡只有一个快峰和一个慢峰; 在加热熔解过程中慢峰分裂为两个峰。慢极化响应和液体中分子的局部束缚空间电荷有关; 慢极化介电谱可以给出分子动力的许多信息。     

N-甲基咪唑衍生物的原位紫外光谱电化学行为

用循环伏安法(CV)测定了寡聚酰胺单体N-甲基咪唑衍生物的电化学行为, 探讨用原位紫外光谱法对电化学反应过程进行检测, 观察到随极化电势的增加在紫外光谱中出现新的吸收峰, 分析了N-甲基咪唑衍生物的还原历程.     

中温固体氧化物燃料电池NiO/YSZ阳极的还原过程

以氢气程序升温还原(H2-TPR)为手段,研究了中温固体氧化物燃料电池烧结NiO/YSZ阳极的还原过程,并通过对电池开路电位和阻抗的原位监测考察了电池中阳极的还原过程.H2-TPR结果表明,阳极烧结温度升高,阳极中的NiO变得难以还原,但当温度提高到1 500℃时,NiO还原峰的峰温降低.阳极NiO含量越高,NiO越容易被还原.这是由于烧结过程中NiO颗粒长大和NiO/YSZ界面分离共同作用的结果.电池原位还原过程中开路电位的变化表明,具有高NiO含量的阳极还原较慢.这主要是由于高NiO含量的阳极具有较大的收缩率和大的NiO粒子,导致还原初期产生的大量H2O不能被及时排出,从而抑制了还原过程.电池还原过程中交流阻抗谱的变化表明,50%NiO/YSZ阳极具有最稳定的还原过程.30%和70%NiO/YSZ电池都有一个极化电阻逐渐增大的过程,前者的极化电阻在还原600 min后逐渐稳定,而后者并不能稳定.     

聚2,6-萘二甲酸乙二醇酯β松弛的热释电研究

本文用短路热释电方法研究了聚萘酯(PEN)的β松弛过程。极化场强和电极效应的实验结果表明,PEN的TSC图谱中50℃的β松弛过程是偶极松弛过程。并且此松弛峰电流值随样品结晶度的增加而降低。用“初始升高法”计算得到其松弛活化能约为0.34eV,且不受结晶度变化的影响。这些实验结果说明β松弛是非晶区小链段的局部运动。     

芪类分子掺杂极化聚合膜的非线性光学性质

采用实时测量光学二次谐波产生（SHG）和吸收光谱的方法时芪类有机分子DANS（4’－N,N－dimethylamino－nitrostilbene）及一种新合成的经氰基团修饰的有机分子CNDS（α’－cyano－4’－nitro－4－N,N－dimethylaminostilbene）掺杂PMMA[poly（methylmethacrylate）]极化聚合膜的非线性光学性质进行了研究。在电晕极化条件下,由于聚合膜的电导率随温度的变化急剧增加,实验中发现两种掺杂极化聚合膜的最佳电导极化温度均低于它们的玻转温度Tg．在最佳极化条件下,从极化前和极化后的吸收光谱变化可看出CNDS的有序度较DANS的差．但实时SHG表明,CNDS／PMMA极化掺杂聚合膜的二阶非线性系数X（2）较DANS／PMMA极化聚合膜的大．结合极化前和极化后吸收峰强度的变化,我们得到CNDS分了的非线性极化率β约为140×10-30esu.在撤离极化场后,CNDS／PMMA的SHG强度的弛豫也比DANS／PMMA慢,说明CNDS是一种性能较DANS优越的制备二阶光学非线性的掺杂分子．     

三聚噻吩的表面光电压谱研究

采用表面光电压和电场诱导表面光电压技术研究了三聚噻吩在外电场作用下的电子运动行为,结合三聚噻吩的UV光谱、极化子概念以及前线轨道理论,指认了三聚噻吩能级跃迁性质,即380nm附近的峰为带－带跃迁峰,477,465和600nm附近的峰是与单极化子有关的电子跃迁;而在770和990nm附近的峰则是与双极化子有关的电子跃迁峰。     

聚芳醚酮在溶液中的分子构象与分子极化

经从头计算,得到4,4'-二氟苯酮二面角为44°,MES₃二面角为51°;用UV光谱法研究了单分散齐聚物在H₂SO₄中的分子构象与极化,结果表明:H₂SO₄使碳基质子化是产生极化的主要因素之一,由此产生的新吸收峰在λ=400nm左右;极化作用产生的平面构象经重叠后在λ=500nm左右产生另一新的吸收峰.由质子化模型并考虑组态相互作用的计算结果与文献一致.证明了聚芳醚酮高聚物在H₂SO₄中,于400nm左右处产生的峰(UV)为羰基极化的结果,指明在H₂SO₄中测其分子量时应按羰基含量校正.     

Mg_(2-x)La_xNi及Mg_(2-x)Ce_xNi合金的腐蚀性能研究

应用电化学方法研究了Mg2-xLaxNi及Mg2-xCexNi储氢合金的腐蚀性能.恒电位极化和交流阻抗测试表明,经Ce或La取代后的合金,其前者腐蚀电流及电化学极化电阻均随Ce取代量增加而降低,而后者的腐蚀电流却随La取代量的增加而增加,但极化电阻则呈先降后升趋势.合金极化后SEM测试显示,经Ce取代后合金表面较平整,而用La取代的则明显有裂纹.作者认为这主要与La、Ce的氧化物的结构有关.     

硫酸水溶液中聚苯胺的两种极化子

应用自设计现场ESR电解池测量不同电势下的聚苯胺电导率,得到了高信/噪比的ESR谱图.谱线分解发现,在硫酸水溶液中聚苯胺生长的早期阶段存在两种极化子,根据这两种成分的ESR峰宽随电极电势的变化以及它和电导的关联分析,分别被指认为聚苯胺中有序区域和无序区域的极化子.随着掺杂程度的增大,两种极化子都是载流子,同样经历了由Curie自旋到Pauli自旋的转变.这一推论得到ESR饱和实验数据的支持.     

亚硝酸甲酯分子在440nm附近的激光光解

近年来亚硝酸甲酯分子（CHa0NO）的光解动力学研究十分活跃｛‘5］，主要集中在紫外激光的单光子解离的机理，光解过程的矢量相关性质和光解产物的态分布．CH30NO分子的解离能D。（CH30－NO）＝174kJ·mol‘，若单从能量上看，人＜689。的光就能使其解离，但人＞400urn的光解离研究还未见报导．＊H30＊0分子在人＞40onm的强激光场下是充电离还是先解离，是单光子解离还是多光子解离，以及通过哪个电子态解离都不清楚．时间飞行质谱不仅具有质量分辨率高、范围宽，而且响应快，因此适合做光解光电离过程初生态产物的探测．特别是时间飞…     

The influence of different variables on the electrochemical behavior of mild steel in circulating cooling water containing aggressive anionic species

Cyclic voltammetric, potentiodynamic anodic polarization and current–time transient studies were carried out on mild steel in circulating cooling water containing Cl⁻ and SO₄⁻² ions under the effect of different variables such as coolant flow, the availability of oxygen, cooling system temperature, and cooling system pH. The anodic excursion span of mild steel in cooling corrosive solution was characterized by the occurrence of a well-defined anodic peak (A1), while the reverse sweep was characterized by the appearance of two cathodic peaks (C1 and C2). The presence of Cl⁻ and SO₄⁻² ions in cooling water enhance the active dissolution of mild steel and tend to breakdown the passive film and induce pitting attack. The data reveal that increasing flow rate and temperature of cooling solution enhances the anodic peak current density (j _A1) and shifts the pitting potential (E _pit) towards more active values. It is seen that the peak current density of the anodic peak A1 increases and the pitting potential (E _pit) displaced in the noble direction in the aerated solution compared that in de-aerated solution. The pitting corrosion of mild steel by Cl⁻ and SO₄⁻² ions initiates more readily in acidic medium (pH 2.0). It was found that the incubation time (t _i) increase and in turn the pitting corrosion decrease in the order: pH 10 > pH 6.8 > pH 2.0.     

Observation of a chevron hybrid structure in the smectic A phase of a liquid crystal device

Small angle X-ray diffraction experiments show the emergence of a chevron structure on cooling from the nematic phase into the smectic A phase of the commercial mixture S3 (Merck Ltd, UK), in a display device. The chevron angle increases from 0 at the nematicsmectic transition temperature, T NS, to a maximum value of 8.5 , which is reached when the sample is 15 C below T NS. Between 5 C and 15 C below the transition temperature a quasi bookshelf structure emerges, in addition to the prevailing chevron structure; such a structure has not been hitherto reported. There is no further resolvable change in the device structure on cooling lower than T NS -15 C. The chevron structure is due to the combination of layer thinning and fixed surface layers, as confirmed by a comparison of layer spacing calculated from the Bragg angle equation and from the layer thinning equation ( d = d nematic cos delta, where delta is the chevron angle).     

Persistent polarization in polymers. I. Relationship between the structure of polymers and their ability to become electrically polarized

The ability of various polymers to acquire persistent polarization (i.e., to become electrets) was investigated. Polarization was induced in the polymers by two methods: (a) by cooling under a voltage drop and (b) by cooling with flow under pressure. There was found to be an optimum temperature for electret formation by either method. This optimum temperature was roughly 37°C. above T_g when polarization was produced by application of a voltage drop and roughly 57°C. when polarization was produced by flow under pressure. Crystallinity and the nonhomogeneities present in blended polymers were harmful to electret formation, but a small critical amount of ionic impurity was helpful.     

Boson peak of alkali and alkaline earth silicate glasses: influence of the nature and size of the network-modifying cation

The influence of the size of the alkaline earth cation on the boson peak of binary metasilicate glasses, MSiO(3) (M = Mg, Ca, Sr, Ba), has been investigated from vibrational densities of states determined by inversion of low-temperature heat capacities. As given both by C(p)/T(3) and g(ω)/ω(2), the intensity of the boson peak undergoes a 7-fold increase from Mg to Ba, whereas its temperature and frequency correlatively decrease from 18 to 10 K and from 100 to 20 cm(-1), respectively. The boson peak results from a combination of librations of SiO(4) tetrahedra and localized vibrations of network-modifying cations with non-bridging oxygens whose contribution increases markedly with the ionic radius of the alkaline earth. As a function of ionic radii, the intensity for Sr and Ba varies in the same way as previously found for alkali metasilicate glasses. The localized vibrations involving alkali and heavy alkaline earth cations appear to be insensitive to the overall glass structure. Although the new data are coherent with an almost linear relationship between the temperature of the boson peak and transverse sound velocity, pure SiO(2) and SiO(2)-rich glasses make marked exceptions to this trend because of the weak transverse character of SiO(4) librations. Finally, the universality of the calorimetric boson peak is again borne out because all data for silicate glasses collapse on the same master curve when plotted in a reduced form (C(P)∕/T(3))/(C(P)/T(3))(b) vs. T/T(b).     

Thermal conductivity of a polymerizing liquid

Thermal conductivity kappa of seven polymerizing liquids has been measured in real time at different temperatures, and calorimetry and dielectric spectroscopy of one liquid are performed to help interpret the results. As a covalently bonded linear chain or a network structure in the liquid grows, kappa of the Debye equation initially increases with the polymerization time t(polym) as the molecular weight, density, and sound velocity increase, as on cooling a liquid. The measured kappa reaches a maximum and then decreases, thus showing a peak at a certain t(polym) and finally becomes constant, which is not the true behavior of steady state kappa. The dielectric relaxation time of the covalently bonded structure at the t(polym) for the kappa peak is less than 5 s and the extent of polymerization is below the vitrification plateau value. The peak height increases when the pulse time for kappa measurement is increased. An increase in the liquid's temperature shifts the kappa peak to a shorter t(polym). Liquid compositions polymerizing rapidly show a similar shift, and those polymerizing slowly or whose viscosity does not reach a high enough value show a small kappa peak or none. The kappa peak may be an artifact of the time dependence of heat capacity during the pulse time used for the kappa measurement, as proposed for glasses and supercooled liquids, similar to the changes in other properties observed as an artifact of kinetic freezing/unfreezing. For a polymerizing liquid, the peak may additionally arise when the rate of increase in the elastic modulus becomes equal to the rate of decrease in equilibrium Cp. In either case, its appearance does not distinguish the Brownian motions' slowing on polymerization from that on cooling or compressing a liquid.     

Vibrational and configurational heat capacity of poly(vinyl acetate) from dynamic measurements

The complex heat capacity C(p) (*) of poly(vinyl acetate) has been measured at 20.95 mrads modulation frequency during the cooling as well as on heating at 24, 8, and 2 Kh and during cooling at 0.5 Kh. The study is complemented with (the rate-dependent) C(p,app) measured during cooling and heating at 60, 24, and 8 Kh. At low temperatures, the real component of C(p) (*) yields the unrelaxed C(p) or C(p,vib), the vibrational part of C(p). It is found to be indistinguishable from C(p,glass) and lies on a line extrapolated to its equilibrium melt's temperature. At T near T(g),DeltaC(p)(=C(p,melt)-C(p,glass)) shows no detectable contribution from C(p,vib). The finding conflicts with a modified entropy theory calculation [E. A. DiMarzio and F. Dowell, J. Appl. Phys. 50, 6061 (1979)], which had predicted that approximately 27% of DeltaC(p) of poly(vinyl acetate) at T near T(g) is vibrational in origin and the remainder configurational. At T相似文献   

Electroosmotic Transport through a Cation-Exchange Membrane: Effect of the Stirring on the Dependence of the Electroosmotic Permeability on the Temperature

The electroosmotic flux through a cation-exchange membrane has been obtained in different situations. From these measurements, the apparent electroosmotic permeability, W, of a cation-exchange membrane has been determined as a function of the temperature, T, and the stirring rate, v, of the solutions. In all the experimental situations studied, W decreases when v increases, while it can increase or decrease with T depending on the temperature range considered. For this last reason, the (T,W) curves show a minimum whose value and position depend on the experimental conditions established. The influence of the concentration polarization effect in the value of W and in its dependence with v and T is studied and quantified. Copyright 1999 Academic Press.     

Relaxation during polymerization on slow heating and the vibrational heat capacity of the polymers

The real and imaginary components of the complex heat capacity, C(p) (') and C(p) ("), and C(p,app) have been measured in real time during the linear chain polymerization on 12 K/h heating of six different (partially) polymerized states of a stoichiometric mixture of cyclohexylamine and diglycidyl ether of bisphenol A. Their C(p,app) shows a sigmoid shape rise with different onset temperatures T(onset), which is followed by a deep exotherm as the viscosity decreases and further polymerization occurs at different rates. The rates of their enthalpy decrease on polymerization determined by subtracting C(p) (') from C(p,app) differ but C(p) (') and C(p,app) of their final states are the same. The relaxation time increases with polymerization and decreases with an increase in T. C(p) (') rises in a sigmoid shape manner, and C(p) (") shows a peak when the relaxation time of the polymerized state is equal to the inverse of the temperature modulation frequency, whether polymerization occurs or not. The unrelaxed or vibrational heat capacity C(p,vib) of the polymers at T>T(onset) is close to C(p) of their glassy state at T相似文献   

Effect of laser parameters on ultrafast hydrogen migration in methanol studied by coincidence momentum imaging

The effect of intensity, duration, and polarization of ultrashort laser pulses (795 nm, 40-100 fs, and 0.15-1.5 × 10(15) W/cm(2)) on the hydrogen migration in methanol is systematically investigated using Coulomb explosion coincidence momentum imaging. The ratio of the ion yield obtained for the migration pathway CH(3)OH(2+) → CH(2)(+) + OH(2)(+) with respect to the sum of the yields obtained for the migration pathway and for the nonmigration pathway CH(3)OH(2+) → CH(3)(+) + OH(+) exhibits a small (10-20%) but clear dependence on laser pulse properties, that is, the ratio decreases as the laser peak intensity increases but increases when the pulse duration increases as well as when the laser polarization is changed from linear to circular.