33 resultados para primary reaction
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全文分两部分,(1).PsⅡ反应中心色素分子光破坏的分子机理研究;(2).PSⅡ反应中心原初反应的动力学机理研究。 在第一部分中,在分离纯化的光系统Ⅱ反应中心Dl/D2/Cyt b559复合物中,采用高效液相色谱技术,首次发现PSⅡ反应中心去镁叶绿素分子的光照破坏,研究了去镁叶绿素的光破坏机理,观察到PsⅡ反应中心内部存在一个与光化学活性无关的去镁叶绿素分子,从而提供了PSⅡ反应中心存在两条电子传递链的第一个实验证据,提出了去镁叶绿素对PsⅡ反应中心的光保护假说和光合作用反应中心第二条电子传递支路的光保护假说。用高效液相色谱技术还观察到PSⅡ反应中心的6个叶绿素a分子,有三种不同的存在状态,认为PSl反应中心的最小色素组成为每个反应中心含有4个叶绿素a和2个去镁叶绿素。用光破坏的方法证明PsⅡ原初电子供体P680是由两个叶绿素n分子组成,认为P680是以一个二聚体形式存在,首次发现P680的光破坏过程包含失去中心镁原子的反应。 在第二部分中,用皮秒和飞秒时间分辨光谱技术,在PsⅡ颗粒、PsⅡ核心复合物和PSⅡ反应中心三个层次上,研究了PsⅡ原初反应的动力学性质,着重研究电荷分离和PsⅡ反应中心内部的能量传递过程。结果表明,B-胡萝卜素和P680之间的能量传递时间常数为350p8左右,去镁叶绿素a与P680之间的能量传递时间为lOOp8左右,提出了可能的动力学模型。 在目前分歧最大的原初电荷分离时间常数测定这一焦点问题上,得到的初步结果表明PsⅡ反应中心电荷分离时间为3-3.5pa左右,这一结论与文献上报道的21pa不同,丽倾向于支持国际上3p8的观点。
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本论文在国内首次利用飞秒吸收光谱技术对PSII颗粒和PSII 核心复合物两个不同层次的PSII样品的原初反应过程进行了研 究。实验采用 400nm 激发, 520~700nm探测,时间分辨率为 120fs。通过多指数拟合和全局分析,对不同波长下的多条衰减 曲线同时采用一套时间组分进行解析,得到了不同波长下的各个 组分的衰减相关差异吸收谱(DADS)。 在 PSII 颗粒的研究中,通过对所有衰减曲线进行数据拟合,解析出了0.16ps、2.8ps、8.6ps、20.9ps、38.8ps和一个非衰减的组分。分析它们各自在520nm~700nm范围内的不同吸收变 化特点,我们得到以下结论: 1.在LHCII中,同一单体同一层中的Chlb与Chla分子之间 的能量传递时间常数约为0.16ps左右; 2.LHCII同一单体中,同一层中的Chla分子之间的能量传递时间常数约为 2.8ps 左右。这与在纯化的 LHCII研究中认为的一3ps组分为不同层的 Chlb→Chla的能量传递过程不同; 3.在PSII颗粒中,8.6ps 组分是与光化学过程有关的时间常数,它可能是从 LHCII 色素蛋白复合物向反应中心等的能量传递及在反应中心中的原初电荷分离过程的平均时间常数; 4.LHCII中不同单体之间的Chla之间的能量传递时间常数约为20.9ps。 在PSII核心复合物的研究中,通过对所有衰减曲线进行数据拟合,解析出了0.35ps、2.9ps、11.2ps、20.lps、36.5ps和一个非衰减的组分。分析它们各自在520nm~700nm范围内的不同吸收变化特点,并与PSII颗粒复合物所得结果相比较,我们得出以下结论: 1.PSII内周天线中相邻 Chla 之间的能量传递时间常数约为 0.35ps左右,这比LHCII中相邻Chlb与Chla之间的能量传递时间常数( 0.16ps )要长;这说明内、外周天线色素蛋白复合物 具有不同的色素空间排列。可以预见在PSII核心天线中相邻叶绿素分子之间的距离要比 LHCII中相邻叶绿素分子的8.3—10.5A 的距离要大一些。这在以前的研究中,并没有见到报导; 2.PSII内周天线中不相邻的Chla之间的能量传递时间常数 约为11.2ps; 3.在PSII核心复合物研究中,2.9ps 和 20.lps 两个组分均与光化学反应过程有关,推测原初电荷分离过程可能是有辅助叶绿 素分子参与的两步反应。
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The catalytic mechanism for the oxidation of primary alcohols catalyzed by the two functional models of galactose oxidase (GOase), M-II L (M = Cu, Zn; L = N,N'-bis(3,5-di-tert-butyl-2-hydroxyphenyl)1-2-diiminoquinone)), has been studied by use of the density functional method B3LYP The catalytic cycle of Cu- and Zn-catalysts consists of two parts, namely, substrate oxidation (primary alcohol oxidation) and O-2 reduction (catalyst regeneration). The catalytic mechanisms have been studied for the two reaction pathways (route 1 and route 2). The calculations indicate that the hydrogen atom transfer within the substrate oxidation part is the rate-determining step for both catalysts, in agreement with the experimental observation.
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Alumina and alumina/mullite composites with mullite content of 0.96-8.72 vol.% were subjected to an abrasive wear test under loads of 0.1-2.0 N with a ball-on-disc apparatus. The wear rate and area fraction of pullout f(po) on the worn surfaces were measured. The wear resistances of the alumina/mullite composites were better by a factor of 1-2 than that of pure alumina. The main wear mechanism of alumina is fracture wear, and for alumina/mullite composites, fracture wear and plastic wear mechanisms work together. The influence of mechanical properties on wear resistance was estimated by Evans' method. It was found that the wear rate depends on f(po), and the primary reason for the better wear resistance of alumina/mullite composites is the reduction off, induced by fracture mode transition. (c) 2007 Elsevier B.V. All rights reserved.
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Extraction kinetics of thorium(IV) with primary amine N1923 in sulfate media has been investigated by a constant interfacial cell with laminar flow. Studies of interfacial tension and effects of the stirring rate, temperature, and specific interfacial area on mass transfer rate show that the most probable reaction zone takes place at the liquid-liquid interface. According to the experimental data correlated as a function of the concentration of the relevant species involved in the extraction reaction, the rate equation of extracting thorium has been obtained as follows: -d[Th(IV)]((o))/dt = 10(-3.10)center dot[Th(IV)](0.89)center dot[(RNH3)(2)SO4](0.74).
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A novel path of preparing PP/o-MMT nanocomposites, which pay attention to the breaking up of MMT original agglomerates and dispersing of its primary particles, rather than the intercalation or exfoliation degree of o-MMT, was reported. The method of predispersing the o-MMT particles into a polar poly(vinyl alcohol) (PVA) matrix and then melt blending the pre-treated PVA/o-MMT hybrids with PP was studied. 3-isopropenyl-alpha,alpha-dimethylbenzene-isocyanate (TMI) was used as a modifier of PVA to improve the compatibility between PVA and PP matrix. Pre-disperse o-MMT with TMI modified PVA was proved to be an effective way to get a composite with fine o-MMT particles dispersion. But the method, which is pre-dispersing o-MMT with non modified PVA and then using TMI to modify such PVA/o-MMT hybrid, would largely reduce the reaction degree between TMI and PVA because of the relatively lower reaction temperature. Although the latter method also can obtain finer dispersion composites than that with using PP-g-MAH as compatibilizer, the relatively higher degradation degree of PP matrix in this method will limit the use of this nanocomposite.
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A new method for synthesis of novel hyperbranched poly(ester-amide)s from commercially available AA' and CBx type monomers has been developed on the basis of a series of model reactions. The hyperbranched poly(ester-amide)s with multihydroxyl end groups are prepared by thermal polycondensation of carboxyl anhydrides (AA') and multihydroxyl primary amine (CBx) without any catalyst and solvent. The reaction mechanism in the initial stage of polymerization was investigated with in situ H-1 NMR. In the initial stage of the reaction, primary amino groups of 2-amino-2-ethyl-1,3-propanediol (AEPO) or tris(hydroxymethyl)aminomethane (THAM) react rapidly with anhydride, forming an intermediate which can be considered as a new AB(x) type monomer. Further self-polycondensation reactions of the AB. molecules produce hyperbranched polymers. Analysis using H-1 and C-13 NMR spectroscopy revealed the degree of branching of the resulting polymers ranging from 0.36 to 0.55. These hyperbranched poly(ester-amide)s contain configurational isomers observed by C-13 and DEPT C-13 NMR spectroscopy, possess high molecular weights with broad distributions and display glass-transition temperatures (T(g)s) between 7 and 96 degreesC.
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2-(2-Phenyl-1H-phenanthro-[9,10-d]imidazole-1-yl)-acetic acid (PPIA) and 2-(9-acridone)-acetic acid (AAA), two novel precolumn fluorescent derivatization reagents, have been developed and compared for analysis of primary aromatic amines by high performance liquid chromatographic fluorescence detection coupled with online mass spectrometric identification. PPIA and AAA react rapidly and smoothly with the aromatic amines on the basis of a condensation reaction using 1-ethyl-3-(3dimethylaminopropyl)-carbodiimide (EDC) as dehydrating catalyst to form stable derivatives with emission wavelengths at 380 and 440 nm, respectively. Taking six primary aromatic amines (aniline, 2-methylaniline, 2-methoxyaniline, 4-methylaniline, 4-chloroaniline, and 4-bromoaniline) as testing compounds, derivatization conditions such as coupling reagent, basic catalyst, reaction temperature and time, reaction solvent, and fluorescent labeling reagent concentration have also been investigated. With the better PPIA method, chromatographic separation of derivatized aromatic amines exhibited a good baseline resolution on an RP column. At the same time, by online mass spectrometric identification with atmospheric pressure chemical ionization (APCI) source in positive ion mode, the PPIA-labeled derivatives were characterized by easy-to-interpret mass spectra due to the prominent protonated molecular ion m/z [M + H](+) and specific fragment ions (MS/MS) m/z 335 and 295. The linear range is 24.41 fmol-200.0 pmol with correlation coefficients in the range of 0.9996-0.9999, and detection limits of PPIA-labeled aromatic amines are 0.12-0.21 nmol/L (S/N = 3). Method repeatability, precision, and recovery were evaluated and the results were excellent for the efficient HPLC analysis. The most important argument, however, was the high sensitivity and ease-of-handling of the PPIA method. Preliminary experiments with wastewater samples collected from the waterspout of a paper mill and its nearby soil where pollution with aromatic amines may be expected show that the method is highly validated with little interference in the chromatogram.
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采用高精度的ENO格式和基于基元化学反应的真实化学反应模型求解氢氧混合气体一维爆轰波的精细结构。采用直接起爆方法得到稳定传播的爆轰波,计算的爆轰波阵面参数和实验相当符合。对爆轰波反应区化学反应的研究表明,参与反应的不同组分具有不同类型的变化特征。网格尺寸影响的研究表明,计算结果的精度随着网格尺寸的增加而增加,并能保持较好的收敛性。移动网格研究结果表明,网格运动速度和爆轰速度接近时,两者的相互作用对计算结果产生一定影响。
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A chemical oxygen iodine laser (COIL) that operates without primary buffer gas has become a new way of facilitating the compact integration of laser systems. To clarify the properties of spatial gain distribution, three-dimensional (3-D) computational fluid dynamics (CFD) technology was used to study the mixing and reactive flow in a COIL nozzle with an interleaving jet configuration in the supersonic section. The results show that the molecular iodine fraction in the secondary flow has a notable effect on the spatial distribution of the small signal gain. The rich iodine condition produces some negative gain regions along the jet trajectory, while the lean iodine condition slows down the development of the gain in the streamwise direction. It is also found that the new configuration of an interleaving jet helps form a reasonable gain field under appropriate operation conditions. (c) 2007 Elsevier Ltd. All rights reserved.
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In this paper we deduce the formulae for rate-constant of microreaction with high resolving power of energy from the time-dependent Schrdinger equation for the general case when there is a depression on the reaetional potential surface (when the depression is zero in depth, the case is reduced to that of Eyring). Based on the assumption that Bolzmann distribution is appropriate to the description of reactants, the formula for the constant of macrorate in a form similar to Eyring's is deduced and the expression for the coefficient of transmission is given. When there is no depression on the reactional potential surface and the coefficient of transmission does not seriously depend upon temperature, it is reduced to Eyring's. Thus Eyring's is a special case of the present work.
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This study focuses on mechanism of ceramic coating on Al-Si alloys with bulk primary Si using plasma electrolytic oxidation (PEO) technology. Al-Si alloys with 27-32% Si in weight were used as substrates. The morphologies, composition and microstructure of PEO coatings were investigated by scanning electron microscopy (SEM) with energy dispersive X-ray system (EDX). Results showed that the PEO process had four different stages. The effect of bulk Si is greatly on the morphology and composition of coatings at first three stages. Anodic oxide films formed on Al and Si phases, respectively. When the voltage exceeded 40 V, glow appeared and concentrated on the localized zone of interface of Al and Si phase. Al-Si-O compounds formed and covered on the dendrite Si phase surface, and the coating on bulk Si, which was silicon oxide, was rougher than that on other phase. If the treatment time was long enough, the coatings with uniform surface morphologies and elements distribution will be obtained but the microstructure of inner layer is looser due to the bulk Si.
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The primary and secondary threshold intensities of ultraviolet-laser-induced preferential domain nucleation in nearly stoichiometric LiTaO3 is observed. The primary threshold is the minimum intensity to achieve the instantaneous preferential domain nucleation within the focus by the combined action of irradiation and electric fields. The secondary threshold is the minimum intensity to achieve the memory effect without any irradiation within the original focus. The space charge field created by the photoionization carriers is thought to be responsible for the instantaneous effect. The explanation based on the formation and transformation of extrinsic defect is presented for the memory effect. (c) 2008 American Institute of Physics.