由聚苯胺粒子组成的电流变液的研究

由经碱处理的掺杂态聚苯胺（ＰＡｎ）制得高介电常数的半导体ＰＡｎ粒子，将其悬浮于电绝缘油可组成电流变液，讨论了电流变（ＥＲ）液的静态屈服应力（τ＿ｓ），电流密度等性能与ＰＡｎ的介电常数（ε＿ｐ），导电率（σ），体积分数和应用电场强度的关系。对导电率相同的ＰＡｎ粒子，用氨水处理的ＰＡｎ粒子ε＿ｐ较用ＮａＯＨ液处理的高，前者在σ足够低如σ≤１．０×１０￣（－７）／ｃｍ时，ＥＲ液的τ＿ｓ随偶极系数的平方（β￣２）的增大而呈现非线性增加；后者ＥＲ液的τ＿ｓ随β￣２的增大出现一最大值．结果表明：由聚苯胺粒子可组成高电流变活性的无水ＥＲ液．     

Ce1－xPrxO2－δ (x＝0.05～0.30)固溶体的合成及其性质研究

利用溶胶-凝胶法合成了固溶体Ce1－xPrxO2－δ (x＝0.05～0.30). X射线衍射(XRD)分析表明, 在x≤0.30的范围内形成了单相萤石结构固溶体Ce1－xPrxO2－δ; X射线光电子能谱(XPS)结果表明, 样品中氧缺位浓度随掺杂量增大而增大, 铈离子主要为Ce4＋离子, 镨离子以混合价态Pr3＋和Pr4＋存在; 拉曼光谱(Raman)观察到两个峰, 458 cm－1峰为特征F2g振动谱带, 较宽的570 cm－1峰与样品中氧离子缺位有关; 交流阻抗谱测试表明, 固溶体Ce1－xPrxO2－δ的电导率随掺杂量增加而增大, x＝0.2时, 电导率达到最大, 活化能较低, σ600 ℃＝3.28×10－2 S/cm, σ700 ℃＝6.06×10－2 S/cm, Ea＝0.54 eV (250～650 ℃), Ea＝0.49 eV (650～800 ℃).     

N-丙烯酰吗啉在可聚合叔胺-过硫酸钾水溶性引发体系引发下的水溶液聚合

本文报道了以甲基丙烯酸－N，N－甲氨基乙酯（DMAEMA）与过硫酸盐体系以引发的丙烯酰吗啉（AMP）的水溶液聚合，得到下列方程：Rp［K2S2O8］0．46［DMAEMA］0．49［AMP］1．09；Ea＝30．21KJ／mol。试用四氯乙烯（TCNE）处理的丙烯酸吗啉聚合物P（AMP）的紫外光谱分析，发现DMAEMA不仅参与引发AMP聚合，而且还进入P（AMP）分子链中。P（AMP）分子量比聚丙烯酰腹P（AAm）的小，而且随AMP（DMAEMA或温度）增加而增加（降低）。P（AMP）及其轻度交联的水凝胶表现出热敏性。     

高分子电解质溶胶－凝胶相转移与溶剂效应

以溶质、溶剂间的协同作用作为高分子电解质体系的凝胶化条件，以松软粒子结构（Ｂｌｏｂ）间的三维逾渗的凝胶化模型，将高分子电解质体系的凝胶化分为松软粒子的形成和逾渗过程。结合海藻酸溶液的Ｃｕ２＋、Ｃａ２＋、Ｍｎ２＋和Ｃｏ２＋离子添加体系的凝胶化，分析了高分子电解质溶胶－凝胶相转移的实质，得到了体系相对粘度的临界指数ｋ＝０．９０～１．１４，与逾渗模型的预测值相吻合，探讨了松软粒子的形成对相转移临界点ｆｃ的影响，明确了临界点附近相对粘度的幂次公式ηｒｅｌ∝（ｆｃ—ｆ）－ｋ）的适用范围。     

Fe/MnO-ZnZSM-5双功能催化剂上合成气直接转化为芳烃的反应

 探讨了Fe／MnO－ZnZSM－5（n（SiO2）／n（Al2O3）＝50）双功能催化剂上合成气直接转化为芳烃的反应，考察了反应温度和Zn载量对CO转化率及芳烃选择性的影响．结果表明，Fe／MnO－ZnZSM－5具有良好的合成气芳构化性能，在V（CO）∶V（H2）∶V（Ar）＝3∶6∶1，SV＝1600h－1，p＝1．1MPa，T＝543K的条件下，CO转化率可达到98．1％，芳烃产物选择性可高达53．1％．催化剂经60h运转后，CO转化率仅降低0．5％，显示了良好的稳定性和应用前景．     

Ar离子束作用下C60薄膜的结构稳定性研究

利用XPS和AES研究了在Ar离子束作用下C60薄膜的分子结构的稳定性．研究发现C60分子与Ar离子束作用后，C1s结合能从284．7eV逐步下降到284．4eV，CKLL俄歇动能从270．0eV增加到271．3eV．并且C60薄膜在与氩离子束作用后，其C60分子结构特征的C1s携上峰及价带峰均消失．表明Ar离子束可以促使C60分子的C＝C双键断裂，离域π键消失，C60分子分解为单质碳．C＝C双键断裂过程与离子束的能量和辐照时间有一定的函数关系．     

聚1-三甲基硅基丙炔膜渗透汽化分离乙醇-水溶液的研究Ⅰ.PTMSP膜渗透汽化分离乙醇-水传质的基本特征

研究了聚１－三甲基硅基丙炔膜渗透汽化分离乙醇－水溶液传质的主要特点。发现膜对乙醇优先吸附、溶解，对水优先扩散。但因吸附液中水含量很低，总的结果表现为优先透醇。在３１３Ｋ，膜厚２０～２５μｍ，料液浓度１０ｗｔ％时，α＝１８．５，Ｊ＝０．９６９ｋｇ·ｍ－２·ｈ－１。透过膜的渗透液及其中的水和乙醇渗透汽化表观活化能分别为２８．８７、３１．３０和２７．６６ｋＪ／ｍｏｌ，并随料液浓度下降而增加。对实验数据进行非线性回归，建立了该膜传递乙醇的经验关联式：Ｊｅ＝－５．５６４Ｃ２Ｅ０＋１３．３４ＣＥ０－０．１５７３（ｋｇ·ｍ－２·ｈ－１），计算值与实验值相吻合。     

新型St—Co—DMAEMA共聚物的合成与表征

本文研究了苯乙烯（St，M1）与N、N－二甲胺基甲基丙烯酸乙酯（MAEMA，M2）以AIBN为引发剂，在丁酮溶液中的共聚合反应。用元素分析法测定了共聚物的组成，同时分别用FR法、YBR法和K－T法对单体竞聚率进行估价。结果表明三种计算方法得到的单体竞聚率基本一致，结果分别为r1＝0．510，r2＝0．716（FR法）；r1＝0．512，r2＝0．720（YBR法）；r1＝0．505，r2＝0．697（K－T法）。     

乙烯基聚硅氧烷共聚反应竞聚率的测定及其对复合粒子形态的影响

用Ｆｉｍｅｍａｎ－Ｒｏｓｓ法处理数据，测定了乙烯基聚硅氧烷（ＳＶ）与苯乙烯（ＳＴ）、甲基丙烯酸甲酯（ＭＭＡ）和甲基丙烯酸正丁酯（ｎ－ＢＭＡ）的共聚反应的竞聚率，结果为ｒＳＴ＝１．４５和ｒＳＶ＝１．０８，ｒＭＭＡ＝０．７８和ｒＳＶ＝２．０１，ｒｎ－ＢＭＡ＝０．４６和ｒＳＶ＝３．４９．以含ＳＶ的乳液作为种子进行烯类单体的乳液聚合，单体和ＳＶ共聚反应对复合粒子的形态有很大影响。     

钛硅分子筛在环己酮肟气相贝克曼重排反应中的失活

 对比了不同孔径的钛硅分子筛催化剂Ti－MCM－41（Si／Ti摩尔比＝27）和TS－1（Si／Ti摩尔比＝25）对环己酮肟气相贝克曼重排反应的催化性能，分析了它们在重排反应中的积碳量和孔体积的变化．结果表明，这些钛硅分子筛催化剂的失活主要是由积碳引起的，且积碳速率受催化剂孔径的制约．在重排反应过程中，TS－1催化剂微孔孔道内的积碳量随反应时间线性增加，微孔体积随反应时间线性下降；而二次孔内的积碳量随反应时间呈指数增加，孔体积随反应时间呈指数递减．     

On the relation between the activation energy for electron attachment reactions and the size of their thermal rate coefficients

Rate coefficients k(T) for dissociative electron attachment (DEA) to molecules in many cases exhibit a more or less strong rise with increasing temperature T (the electron temperature T(e) and the molecular temperature T(G) are assumed to be in thermal equilibrium, i.e., T = T(e) = T(G)). This rise is frequently modeled by the Arrhenius equation k(T) = k(A) exp[-E(a)∕(k(B)T)], and an activation energy E(a) is deduced from fits to the experimental data k(T). This behavior reflects the presence of an energy barrier for the anion on its path to the dissociated products. In a recent paper [J. Kopyra, J. Wnorowska, M. Forys?, and I. Szamrej, Int. J. Mass Spectrom. 268, 60 (2007)] it was suggested that the size of the rate coefficients for DEA reactions at room temperature exhibits an exponential dependence on the activation energy, i.e., k(E(a); T ≈ 300 K) = k(1) exp[-E(a)∕E(0)]. More recent experimental data for molecules with high barriers [T. M. Miller, J. F. Friedman, L. C. Schaffer, and A. A. Viggiano, J. Chem. Phys. 131, 084302 (2009)] are compatible with such a correlation. We investigate the validity and the possible origin of this dependence by analyzing the results of R-matrix calculations for temperature-dependent rate coefficients of exothermic DEA processes with intermediate barrier toward dissociation. These include results for model systems with systematically varied barrier height as well as results of molecule-specific calculations for CH(3)Cl, CH(3)Br, CF(3)Cl, and CH(2)Cl(2) (activation energies above 0.2 eV) involving appropriate molecular parameters. A comparison of the experimental and theoretical results for the considered class of molecules (halogenated alkanes) supports the idea that the exponential dependence of k(T = 300 K) on the activation energy reflects a general phenomenon associated with Franck-Condon factors for getting from the initial neutral vibrational levels to the dissociating final anion state in a direct DEA process. Cases are discussed for which the proposed relation does not apply.     

Dissociation energetics and mechanisms of leucine enkephalin (M+H)+ and (2M+X)+ ions (X=H, Li, Na, K, and Rb) measured by blackbody infrared radiative dissociation

The dissociation kinetics of protonated leucine enkephalin and its proton and alkali metal bound dimers were investigated by blackbody infrared radiative dissociation in a Fourier-transform mass spectrometer. From the temperature dependence of the unimolecular dissociation rate constants, Arrhenius activation parameters in the zero-pressure limit are obtained. Protonated leucine enkephalin dissociates to form b(4) and (M-H(2)O)(+) ions with an average activation energy (E(a)) of 1.1 eV and an A factor of 10(10.5) s(-1). The value of the A factor indicates that these dissociation processes are rearrangements. The b(4) ions subsequently dissociate to form a(4) ions via a process with a relatively high activation energy (1.3 eV), but one that is entropically favored. For the cationized dimers, the thermal stability decreases with increasing cation size, consistent with a simple electrostatic interaction in these noncovalent ion-molecule complexes. The E(a) and A factors are indistinguishable within experimental error with values of ~1.5 eV and 10(17) s(-1), respectively. Although not conclusive, results from master equation modeling indicate that all these BIRD processes, except for b(4) --> a(4), are in the rapid energy exchange limit. In this limit, the internal energy of the precursor ion population is given by a Boltzmann distribution and information about the energetics and dynamics of the reaction are obtained directly from the measured Arrhenius parameters.     

Electron paramagnetic resonance investigation of the electron-doped manganite La(1-x)Te(x)MnO3 (0.1 ≤ x ≤ 0.2)

The electron paramagnetic resonance (EPR) properties of the electron-doped manganite La(1-x)Te(x)MnO(3) (0.1 ≤ x ≤ 0.2) are investigated based on the data of EPR spectra, resistivity, and magnetic susceptibility. With decreasing temperature from 400 K, the EPR linewidth ΔH(PP) decreases and passes through a minimum at T(min), then substantially increases with further decreasing temperature. The broadening of the EPR linewidth above T(min) can be understood in terms of the increase in the relaxation rate of spin of e(g) polarons to the lattice with increasing temperature due to the similarity between the temperature dependence of the linewidth ΔH(pp)(T) and the conductivity σ(T). For the samples with x = 0.1 and 0.15, the conductivity activation energy E(σ) is comparable with the activation energy E(a) deduced from the linewidth. Whereas for the x = 0.2 sample, there is a large difference between E(σ) (0.2206 eV) and E(a) (0.0874 eV).     

Adsorption of CO2 on oxidized, defected, hydrogen and oxygen covered rutile (1 x 1)-TiO2(110)

Presented are initial, S(0) and coverage, Theta, dependent S(Theta), adsorption probability measurements of CO(2) as a function of impact energy, E(i) = 0.12-1.3 eV, adsorption temperature, T(s) = 85-300 K, hydrogen and oxygen pre-exposure, as well as density of defects, Gamma, as varied by annealing (T = 600-900 K) and Ar(+) ion sputtering (dose chi(Ar) at 600 eV at 85 K) of a rutile (1 x 1) TiO(2)(110) surface. The defect densities were qualitatively characterized by thermal desorption spectroscopy (TDS) of CO(2). The CO(2) TDS curves consisted of two structures that can be assigned to adsorption on pristine and oxygen vacancy sites, in agreement with earlier studies. S(0) decreased linearly with E(i) and was independent of T(s). The adsorption dynamics were dominated by the effect of precursor states leading to Kisliuk-like shapes over the E(i) and T(s) range studied. Oxygen vacancy sites reduced S(0) of CO(2). Preadsorbed oxygen blocked preferentially defect sites, which led to an increase in S(0). Hydrogen preadsorption results in physical site blocking with decreased S(0) as H-preexposure increased, while the shape of S(Theta) curves was conserved. In contrast to oxygen, hydrogen does not adsorb preferentially on defect sites. The adsorption probability data were parameterized by analytic functions (Kisliuk model) and by Monte Carlo simulations (MCSs).     

Dissociative recombination of the deuterated acetaldehyde ion, CD3CDO(+): product branching fractions, absolute cross sections and thermal rate coefficient

Dissociative recombination of the deuterated acetaldehyde ion CD3CDO(+) has been studied at the heavy-ion storage ring CRYRING, located at the Manne Siegbahn Laboratory, Stockholm, Sweden. Product branching fractions together with absolute DR cross-sections were measured. The branching fractions were determined at a relative collision energy between the ions and the electrons of approximately 0 eV. With a probability of 34% the DR events resulted in no ruptures of bonds between heavy atoms (i.e. no breakage of the C-C bond or the C[double bond, length as m-dash]O bond). In the remaining 66% of the events one of the bonds between the heavy atoms was broken. The energy-dependent cross-section for the DR reaction was measured between approximately 0 and 1 eV relative kinetic energy. In the energy region between 1 meV and 0.2 eV the absolute cross section could be fitted by the expression sigma(E) = 6.8 x 10(-16)E(-1.28) cm(2), whereas in the energy interval between 0.2 and 1 eV the data were best fitted by sigma(E) = 4.1 x 10(-16)E(-1.60) cm(2). From these cross section data the thermal rate coefficient (as a function of the electron temperature), alpha(T) = 9.2 x 10(-7) (T/300)(-0.72) cm(3) s(-1) was obtained.     

The dependence of low-energy electron attachment to CF3Br on electron and vibrational energy

In a joint experimental and theoretical effort, we have studied dissociative electron attachment (DEA) to the CF3Br molecule at electron energies below 2 eV. Using two variants of the laser photoelectron attachment method with a thermal gas target (T(G) = 300 K), we measured the energy dependent yield for Br- formation over the range E = 3-1200 meV with resolutions of about 3 meV (E < 200 meV) and 35 meV. At the onsets for excitation of one and two quanta for the C-Br stretching mode nu3, downward cusps are detected. With reference to the recommended thermal (300 K) attachment rate coefficient k(A)(CF3Br) = 1.4 x 10(-8) cm3 s(-1), absolute cross sections have been determined for Br- formation. In addition, we studied Br- and (CF3Br)Br- formations with a seeded supersonic target beam (10% CF3Br in helium carrier gas, with a stagnation pressure of 1-4 bars and nozzle temperatures of 300 and 600 K) and found prominent structure in the anion yields due to cluster formation. Using the microwave pulse radiolysis swarm technique, allowing for controlled variation of the electron temperature by microwave heating, we studied the dependence of the absolute DEA rate coefficient on the mean electron energy E over the range of 0.04-2 eV at gas temperatures T(G) ranging from 173 to 600 K. For comparison with the experimental results, semiempirical resonance R-matrix calculations have been carried out. The input for the theory includes the known energetic and structural parameters of the neutral molecule and its anion; the parameters of the resonant anion curves are chosen with reference to the known thermal rate coefficient for the DEA process. For the gas temperature T(G) = 300 K, good overall agreement of the theoretical DEA cross section with the experimental results is observed; moreover, rate coefficients for Br- formation due to Rydberg electron transfer, calculated with both the experimental and the theoretical DEA cross sections, are found to agree with the previously reported absolute experimental values. At T(G) = 300 K, satisfactory agreement is also found between the calculated and experimental attachment rate coefficients for mean electron energies E = 0.04-2 eV. The strong increase of the measured rate coefficients with rising gas temperature, however, could be only partially recovered by the R-matrix results. The differences may result from the influence of thermal excitations of other vibrational modes not included in the theory.     

Dissociative recombination of fully deuterated protonated acetonitrile, CD3CND+: product branching fractions, absolute cross section and thermal rate coefficient

The dissociative recombination of fully deuterated protonated acetonitrile, CD(3)CND(+), has been investigated at the CRYRING heavy ion storage ring, located at the Manne Siegbahn Laboratory, Stockholm, Sweden. Branching fractions were measured at approximately 0 eV relative collision energy between the ions and the electrons and in 65% of the DR events there was no rupture of bonds between heavy atoms. In the remaining 35%, one of the bonds between the heavy atoms was broken. The DR cross-section was measured between approximately 0 eV and 1 eV relative collision energy. In the energy region between 1 meV and 0.1 eV the cross section data were best fitted by the expression sigma = 7.37 x 10(-16) (E/eV)(-1.23) cm(2), whereas sigma = 4.12 x 10(-16) (E/eV)(-1.46) cm(2) was the best fit for the energy region between 0.1 and 1.0 eV. From the cross section a thermal rate coefficient of alpha(T) = 8.13 x 10(-7) (T/300)(-0.69) cm(3) s(-1) was deduced.     

Ultraslow Li diffusion in spinel-type structured Li4Ti5O12 - a comparison of results from solid state NMR and impedance spectroscopy

The cubic spinel oxides Li(1+x)Ti(2-x)O(4) (0 < or =x< or = 1/3) are promising anode materials for lithium-ion rechargeable batteries. The end member of the Li-Ti-O series, Li(4)Ti(5)O(12), can accommodate Li ions up to the composition Li(7)Ti(5)O(12). Whereas a number of studies focus on the electrochemical behaviour of Li insertion into and Li diffusion in the Li intercalated material, only few investigations about low-temperature Li dynamics in the non-intercalated host material Li(4)Ti(5)O(12) have been reported so far. In the present paper, Li diffusion in pure-phase microcrystalline Li(4)Ti(5)O(12) with an average particle size in the microm range was probed by (7)Li solid state NMR spectroscopy using spin-alignment echo (SAE) and spin-lattice relaxation (SLR) measurements. Between T = 295 K and 400 K extremely slow Li jump rates tau(-1) ranging from 1 s(-1) to about 2200 s(-1) were directly measured by recording the decay of spin-alignment echoes as a function of mixing time and constant evolution time. The results point out the slow Li diffusion in non-intercalated Li(4)Ti(5)O(12) x tau(-1) (1/T) follows Arrhenius behaviour with an activation energy E(ASAE) of about 0.86 eV. Interestingly, E(ASAE) is comparable to activation energies deduced from conductivity measurements (0.94(1) eV) and from SLR measurements in the rotating frame (0.74(2) eV) rather than from those performed in the laboratory frame, E(A)(low-T) = 0.26(1) eV at low T.     

Conductivity of carbon black-loaded styrene–butadiene rubber

Styrene–butadiene rubber (SBR) charged with 50 phr of HAF carbon black has been found to show a positive temperature coefficient of resistivity close to 0.07/°C at 27°C. Beyond a point (75°C) of minimum conductivity, however, it behaves as a normal noncrystalline semiconductor with a resistivity which decreases with rise of temperature with an activation energy of 0.56 eV. Blending the composition with poly(vinyl chloride) (PVC) shifts the minimum towards lower temperatures. The descending branch of the conductivity versus reciprocal absolute temperature characteristic is probably associated with thermal expansion of tunnelling paths separating the conducting carbon particles.     

Synthesis and properties of a new polydiacetylene: Poly[1,6-di(N-carbazolyl)-2,4-hexadiyne]

The solid-state synthesis and properties are reported for a new polydiacetylene: poly[1,6-di(N-carbazolyl)-2,4-hexadiyne]. The monomer crystals polymerize quantitatively with γ irradiation or thermal annealing. An Autocatalytic effect is observed in both γ-ray polymerization and thermal polymerization and is attributed to an increase in chain propagation length at about 5% conversion. The activation energy for thermal polymerization is about 25 kcal/mole, independent of the degree of conversion to polymer. The exceptional thermal stability of the polymer crystals allowed a thermomechanical analysis over a large temperature range, ?50 to 300°C. With increasing temperature, the polymer contracts in the chain direction linearly with temperature over the entire range, yielding a thermal expansion coefficient of (?2.32 ± 0.02) × 10^?5°C^?1. Photoconductivity action spectra are reported for the polymer crystals. The energies for the photoconductivity onset (ca. 2.3 eV) and for the lowest energy optical transition (1.89 eV) are the lowest reported for the polydiacetylenes. The photoconduction onset is blue-shifted with respect to optical absorption—a result which is consistent with the excitonic assignment for the lowest energy optical transition in the polydiacetylenes.