全同1，2－聚丁二烯的合成及用~(13)C-NMR方法研究1，2－聚丁二烯的序列结构

采用Cr／Al催化体系，成功地合成了全同1，2－聚丁二烯（PBD），并用DSC方法、X－射线衍射、红外光谱及~(13)C－NMR的方法进行结构与物性测定，得如下结果：全同1，2－PBD的熔点为124.3℃；三角晶系中，分子链成了螺旋，晶胞参数为a＝17.3A，c＝ 6.5A；在红外光谱中，其特征谱带出现在694.4 cm~(-1)处；在~(13)C－NMR谱中仅出现四条谱峰，其化学位移分别为142.51、111.56、39.26、37.43 ppm。全同1，2－PBD的~(13)C－NMR谱提供的实验数据表明，在~(13)C－NMR谱中1，2－PBD－CH二碳十个五元组谱峰的归属是有别于Elgert、Kumar已有的归属。它属于一种新的归属，与半经验方法所推演的结果相符。它恰巧同聚丙烯侧甲基五元组谱峰的归属一致。采用半经验方法研究了1，2－PBD的~(13)C－NMR增中CH二碳五元组、CH_2－碳四元组及六元组共振谱峰，同时讨论了模型链的链长、温度以及立构序列的排列对各立构序列键概率的影响，求得了相应的r值。同时采用经验方法对1，2－PBD的~(13)C－NMR谱中CH_2=碳、CH－碳五元组及CH_2－碳四元组谱峰做了归属。两种方法对CH_2－碳谱峰的归属得到了一致的结果。

氧络铬卟啉配合物的合成结构及其氧化活性研究

本文选择不同配体（苯酚类和迭氮）通过Cr(III)(TPP)Cl (Al)的氧化还原取代，分别合成了四个新的铬（III）卟啉配合物，Cr(TPP)N_3P_Y(B_1), P-O_2NC_6H_4OCr(TPP)·THF (C1), P-CH_3OCoH_4OCr(TPP)·THF (D1), Cr(TPP)OC_6H_5·THF (E1)。通过元素分析，红外光谱、~1H NMR、ESR、MS和UV-Vis等分析、表征，确认了以上四种化合物。B1单晶进行了X－射线分析，得其晶体结构和分子结构，从而进一步证实了B1的组成。在CH_2Cl_2或C_6H_6中，氮气保护下，用PhIO直接氧化以上五种铬（III）卟啉配合物，合成并分离出了相应的高价氧络铬卟啉配合物，(PhI) O=Cr(▽)(TPP)Cl (A2), (PhI) O=Cr(▽)(TPP)N_3, (B2), P-O_2NC_6H_4O Cr(▽)(TPP) (1/2IPh) (C2), P-CH_3OC_6H_4O Cr(▽)(TPP) (1/2IPh) (D2), PhIO- Cr(IV)(TPP) (OC_6H_5)·P_Y (E2)。通过研究其元素组成，IR、UV－Vis、ESR、MS等分析，确定了以上五种化合物的组成。基中PhI和P_Y分子的位置尚无法确定。这两类高价氧络铬卟啉，是继右淑珍等第一次得到P450模型化合物的活性中间体－氧络铬（▽）四苯基卟啉对硝基苯甲酸配合物后，又一次得到的苯酸类和迭氮氧络铬卟啉配合物。不同的是，氧络铬（▽）卟啉配合物中都各有PhI分子，化合物E2是第一次得到的关键氧络铬（IV）卟啉配合物，类似于PhIO－Mn~(IV)(TPP)(P-H_2N C_6H_4 CO_2)。高价氧络铬卟啉配合物不稳定，室温下分解，暴露在空气中同时发生分解和还原。不过低温下比较稳定。在CH_2Cl_2或C_6H_6中，我们研究了上述五种氧络铬及Cr(TPP)ClPhIO对碳氢化合物和DNA碱基的氧化反应。不同摩尔比的PhIO-Cr(TPP)Cl对环已烷的氧化给出相同的产物，但转化率和产物分布不同。Al-PhIO和C_2-PhIO体内对碱基胞嘧啶，胸腺嘧啶，腺嘌呤的氧化反应呈阳性，氧化产物中都有尿素CO(NH_2)_2，其中胸腺嘧啶的氧化产物中含有CH_3CO-或CH_3CHOH。这说明氧络铬卟啉配合物能够氧化DNA碱基。氧络铬卟啉具有较高的氧化活性和立体选择性。比较不同轴向配体的氧络铬卟啉的氧化活性，其大小次序正好与其轴向配体的配位能力次序一致。这是由于轴向配体的给电子能力越强，通过中心离子铬向其周围转移的电荷就越多，导致氧络键的强度减弱，即其活性增加。上述研究结果表明，铬（III）卟啉配合物是P－450的较好的模型化合物，氧络铬卟啉配合物是其活性中间体。同时该研究结果支持了Groves等提出的定居卟啉配合物催化氧化机理。

以邻菲咯啉为配体的铬系催化剂制备1,2-聚丁二烯

以邻菲咯啉(简称Phen)为配体、异辛酸铬(简称Cr)-三异丁基铝(简称Al)为催化剂、己烷为溶剂合成1,2-聚丁二烯,考察了Phen和Al用量以及聚合温度对1,2-聚丁二烯微观结构及其相对分子质量的影响。结果表明,低相对分子质量聚合物是Cr和Al作用的结果,高相对分子质量聚合物是Cr、Phen和Al作用的结果;在Phen/Cr(摩尔比)为1.0、Al/Cr(摩尔比)为20、聚合温度为50℃的条件下,Cr-Phen-Al催化剂具有高活性,可得到1,2-结构摩尔分数约为50%、相对分子质量呈双峰分布、间同度为28%的聚丁二烯。

The synthesis of some 1,1 '-ferrocene dichalcogenato complexes containing chromium, molybdenum and tungsten

Both dinuclear [3] ferrocenophane derivatives of the type Fe(C5H4E)(2)[MLn] [E = S,Se; MLn = Cp* - Cr(NO) (1), Cp* Mo(NO) (2a,2b), CpMo(NO) (3), Cp* W(NO) (4a,4b), Ca2Mo (6b), Cp2W (7a)] and trinuclear 1,1' - ferrocene dichalcogenato complexes Fe(C5H4E)(2)[MLn](2)[MLn = Cp* Cr(NO)(2), E = S(8a), Se(8b)] were synthesized and characterized by their IR, H-1 MMR and EI - MS spectra as well as their elemental analyses.

以水滑石类化合物为前体的Co-M-Al(M=过渡金属)复合氧化物对催化消除NO_x活性的研究

以共沉淀法制得的水滑石类化合物为催化剂前体,经焙烧可得到一系列尖晶石类化合物Co-M-Al[M=Cr,Mn,Fe,Ni,Cu;n(Co):n(M):n(Al)=3:1:1].通过XRD,比表面测定,化学分析,NO吸附等方法对其进行表征,测定了此系列催化剂对NO催化还原和催化分解的活性,结果发现此系列催化剂对消除NO具有很高的活性.同时对催化消除NO的机理及过渡金属离子中d轨道电子对催化活性的影响进行了一些探讨.

层状La-Ba-Cu复合氧化物在CO还原NO反应中活性的研究

氮氧化物是严重的空气污染物,催化消除氮氧化物是环保催化研究的热点问题,在已有报道的催化剂体系中复合氧化物和含铜分子筛受到人们的普遍关注,文献中已有报道ABO_3(A=Ln;B=Cr,Mn,Fe,Co,Ni)型复合氧化物作为CO还原NO反应的催化剂.但迄今尚未见有合成LaCuO_3的报道,有关含铜复合氧化物作催化剂的大多是A_2BO_4型的.呈ABO_3结构的含铜复合氧化物只有成层状的超导体如YBa_2Cu_3O_7,本文为了探讨复合氧化物晶体结构对催化活性的影响,首次研究了3种层状ABO_3结构的La-Ba-Cu复合氧化物对CO还原NO反应的活性,发现它们均具有较高的活性,并首次提出了Ba离子在此反应中的作用.1 实验方法催化剂的制备和Cu价态分析见文献[4,5]CO还原NO反应在固定床流动反应体系中进行,反应管为内径6mm石英管,催化剂粒度为40～80目,用量0.2g,空速为7000h~(-1),原料气为NO7.5×10~(-3),CO8.0×10~(-3),He平衡.采用英国产的Pyc Pan气相色谱分析检测N_2O,CO_2,0.5nm分子筛色谱柱检测NO,CO转化率. H_2-TPR在自制装置上...

“CR-01”6000m自治水下机器人在太平洋锰结核调查中的应用

介绍了“CR 0 1”自治水下机器人的研制背景和系统的特点 ,以及“CR 0 1”在太平洋锰结核调查中的应用情况 ,并对所获得的数据进行了分析

贵州省几个典型金属矿区周围河水的重金属分布特征

为了解矿山的开采、冶炼对周围水环境的影响,对贵州省杉树林铅锌矿、榨子厂铅锌矿、赫章县后河土法炼锌区、万山汞矿周围水体的重金属(Cr、Mn、Fe、Cu、Zn、As、Se、Cd、Pb) 含量进行了测定。结果显示水流对矿区尾渣堆的冲刷可以导致河水中悬浮颗粒物迁移很远,溶解态重金属含量主要受到悬浮颗粒物释放的影响。颗粒物少的河水溶解态重金属含量低,如榨子厂和万山;颗粒物多的河水则溶解态重金属含量高,如杉树林和赫章后河。

A peculiar metal-rich star, HD 135485

Local thermodynamic equilibrium (LTE) absolute and differential abundances are presented for a peculiar metal-rich B-type star, HD 135485. These suggest that HD 135485 has a general enrichment of similar to0.5 dex in all the metals observed (C, N, O, Ne, Mg, Al, Si, P, S, Cl, Ar, Sc, Ti, Cr, Mn, Fe and Sr), except for nickel. The helium enhancement and hence hydrogen deficiency can account for less than or equal to 0.2 dex of this enhancement of metals, with the additional enhancement probably being representative of the progenitor gas. However, some of the metals appear to have greater enhancements, which may have occurred during the star's evolution. The significantly larger nitrogen abundance coupled with a modest helium enhancement observed in HD 135485 indicates that carbon- nitrogen (CN) processed material has possibly contaminated the stellar surface. Neon and carbon enhancements may indicate that helium core flashes have also occurred in HD 135485. Some of the iron-group elements (viz. Mn and Ni) appear to have similar abundance patterns to that of silicon Ap stars, but it is uncertain how these abundance patterns formed if they were not present in the progenitor gas. From a kinematical investigation it is unclear whether this star formed in a metal-rich region as implied by its chemical composition. From its position in the Hertzsprung-Russell diagram, HD 135485 would appear to be an evolved star lying close to or on the horizontal branch.

Boron abundances in B-type stars: A test of rotational depletion during main-sequence evolution

Boron abundances have been derived for seven main-sequence B- type stars from Hubble Space Telescope STIS spectra around the B III lambda2066 line. In two stars, boron appears to be undepleted with respect to the presumed initial abundance. In one star, boron is detectable but is clearly depleted. In the other four stars, boron is undetectable, implying depletions of 1-2 dex. Three of these four stars are nitrogen enriched, but the fourth shows no enrichment of nitrogen. Only rotationally induced mixing predicts that boron depletions are unaccompanied by nitrogen enrichments. The inferred rate of boron depletion from our observations is in good agreement with these predictions. Other boron-depleted nitrogen-normal stars are identified from the literature. In addition, several boron- depleted nitrogen-rich stars are identified, and while all fall on the boron-nitrogen trend predicted by rotationally induced mixing, a majority have nitrogen enrichments that are not uniquely explained by rotation. The spectra have also been used to determine iron group (Cr, Mn, Fe, and Ni) abundances. The seven B-type stars have near-solar iron group abundances, as expected for young stars in the solar neighborhood. We have also analyzed the halo B-type star PG 0832 + 676. We find [Fe/H] = -0.88 +/- 0.10, and the absence of the B III line gives the upper limit [B/H] <-2.5. These and other published abundances are used to infer the star's evolutionary status as a post-asymptotic giant branch star.

Surface Properties and Catalytic Activity of Manganese Ferrospinels

In recent years considerable advances have been achieved in the study of the surface structure and mechanism of action of environmentally benign heterogeneous catalysts. The study entitled as surface properties and catalytic activity of manganese ferrospinels. In the present study we have prepared manganese ferrospinels of general formula Mn(1-x)BxFe2O4 via low temperature controlled co-precipation method. The study employed low temperature co-precipitation method for the preparation ofMn(1-x)BxFe2O4 specimens, where B is a metal cation such as Cr,Co, Ni,Cu and Zn. The catalytic activities of the systems were investigated for liquid-phase benzoylation of aromatic compounds and phenol hydroxylation and for vapour-phase reactions such as aniline alkylation, phenol methylation and ODH of ethylbenzene. The different series of manganese ferrites are proved to be excellent catalysts for various industrially important reactions such as Friedel-crafts benzoylation of aromatic compounds, methylation of aniline and phenol, hydroxylation of phenol and oxidative dehydrogenation of ethylbenzene. Due to the tightening of the environmental regulations, production of diphenols from phenol hydroxylation and reduction of phenolic pollutants in waste waters using these catalysts can be a promising approach because it demands only simple techniques and produce little environmental pollution.

Electronic transitions and bonding properties in a series of five-coordinate “16-electron” complexes [Mn(CO)3(L2)]− (L2=chelating redox-active π-donor ligand)

In this article we present for the first time accurate density functional theory (DFT) and time-dependent (TD) DFT data for a series of electronically unsaturated five-coordinate complexes [Mn(CO)(3)(L-2)](-), where L-2 stands for a chelating strong pi-donor ligand represented by catecholate, dithiolate, amidothiolate, reduced alpha-diimine (1,4-dialkyl-1,4-diazabutadiene (R-DAB), 2,2'-bipyridine) and reduced 2,2'-biphosphinine types. The single-crystal X-ray structure of the unusual compound [Na(BPY)][Mn(CO)(3)(BPY)]center dot Et2O and the electronic absorption spectrum of the anion [Mn(CO)(3)(BPY)](-) are new in the literature. The nature of the bidentate ligand determines the bonding in the complexes, which varies between two limiting forms: from completely pi-delocalized diamagnetic {(CO)(3)Mn-L-2}(-) for L-2 = alpha-diimine or biphosphinine, to largely valence-trapped {(CO)(3)Mn-1-L-2(2-)}(-) for L-2(2-) = catecholate, where the formal oxidation states of Mn and L-2 can be assigned. The variable degree of the pi-delocalization in the Mn(L-2) chelate ring is indicated by experimental resonance Raman spectra of [Mn(CO)(3)(L-2)](-) (L-2=3,5-di-tBu-catecholate and iPr-DAB), where accurate assignments of the diagnostically important Raman bands have been aided by vibrational analysis. The L-2 = catecholate type of complexes is known to react with Lewis bases (CO substitution, formation of six-coordinate adducts) while the strongly pi-delocalized complexes are inert. The five-coordinate complexes adopt usually a distorted square pyramidal geometry in the solid state, even though transitions to a trigonal bipyramid are also not rare. The experimental structural data and the corresponding DFT-computed values of bond lengths and angles are in a very good agreement. TD-DFT calculations of electronic absorption spectra of the studied Mn complexes and the strongly pi-delocalized reference compound [Fe(CO)(3)(Me-DAB)] have reproduced qualitatively well the experimental spectra. Analyses of the computed electronic transitions in the visible spectroscopic region show that the lowest-energy absorption band always contains a dominant (in some cases almost exclusive) contribution from a pi(HOMO) -> pi*(LUMO) transition within the MnL2 metallacycle. The character of this optical excitation depends strongly on the composition of the frontier orbitals, varying from a partial L-2 -> Mn charge transfer (LMCT) through a fully delocalized pi(MnL2) -> pi*(MnL2) situation to a mixed (CO)Mn -> L-2 charge transfer (LLCT/MLCT). The latter character is most apparent in the case of the reference complex [Fe(CO)(3)(Me-DAB)]. The higher-lying, usually strongly mixed electronic transitions in the visible absorption region originate in the three lower-lying occupied orbitals, HOMO - 1 to HOMO - 3, with significant metal-d contributions. Assignment of these optical excitations to electronic transitions of a specific type is difficult. A partial LLCT/MLCT character is encountered most frequently. The electronic absorption spectra become more complex when the chelating ligand L-2, such as 2,2'-bipyridine, features two or more closely spaced low-lying empty pi* orbitals.

Comparação entre os intumescimentos de borracha natural e polibutadieno com alto teor 1,4-cis em solventes (n-octano, ciclo-hexano e esqualeno) e em soluções poliméricas

Amostras de borracha natural foram reticuladas por meio de radiação gama (doses de 2, 4, 6 e 8 MRad) e intumescidas: a) em n-octano, ciclo-hexano e esqualeno; b) em polibutadieno líquido (Mn=1830 g/mol; alto teor 1,4- cis) a 45°C; C) em solução de polibutadieno de baixo peso molecular (M,= 1830 g/mol; alto teor 1,4-cis) em n-octano e ciclo-hexano; d) em solução de polibutadieno de alto peso molecular (Mn= 175.000 g/rnol; alto teor 1,4-cis) emn-octano e ciclo-hexano ; e) em solução de borracha natural (Mn=779.000 g/mol) em ciclo- hexano, a 25°C. Amostras de polibutadieno (alto teor 1,4-cis) foram reticuladas por meio de radiação gama (doses de 1,s; 18 e 25 MRad) e intumescidas: a) em n-octano, ciclo-hexano e esquaieno. Salvo quando mencionado em contrário, as amostras de borracha natural e de polibutadieno foram intumescidas nas temperaturas de 25, 35 e 45°C. A partir dos ensaios de intumescirnento acima mencionados, foram determinadas as solubilidades de borracha natural e de polibutadieno em n-octano, ciclo-hexano e esqualeno através dos parâmetros de Flory-Huggins, calculados com o emprego da equação de Flory-Rehner. Verificou-se a influência da temperatura e da concentração de polimero no gel sobre o valor do parâmetro de Flory-Huggins. Também através desse parâmetro procurou-se determinar a compatibilidade entre borracha natural e polibutadieno. Foi demonstrado que cadeias lineares de baixo peso molecular de polibutadieno conseguem penetrar em amostras reticuladas de borracha natural, quando o peso molecular das cadeias lineares for bem inferior ao do arco de rede Mc das amostras reticuladas. Cadeias lineares de polibutadieno e de borracha natural com peso molecular superior ao do arco de rede da borracha natural reticulada, entretanto, não conseguem penetrar no retículo. Quranto mais alta a concentração da solução externa em moléculas de alto peso molecular, tanto menor é o grau de intumescimento da amostra reticulada.

Comportamento do aco inoxidavel ABNT 304 a corrosao-sob-tensao em solucoes aquosas neutras de nacl a temperatura de ebulicao utilizando a tecnica de carga constante

Estudou-se o comportamento do aço inoxidável ABNT 304 à corrosão-sob-tensão (C.S.T.) em soluções aquosas com 0,1%, 3,5% e 20% de NaCl, na temperatura de 103°C, através de ensaios de carga constante. Com auxílio das técnicas e conceitos de Mecânica de Fratura Linear Elástica e das análises eletroquímicas procurou-se encontrar as condições em que ocorre C.S.T. no sistema aço inoxidável austenítico/solução aquosa de NaCl a 103°C. Utilizou-se o corpo-de-prova do tipo dupla viga em balanço (T-notch double cantilever beam: TN-DCB), com intuito de observar a influência do fator de intensidade de tensão, concentração da solução e potencial eletroquímico. Estimou-se o valor do fator de intensidade de tensão limite (KICST) e a velocidade de propagação das trincas; também foram analisadas outras importantes características em termos mecanísticos. Definiu-se faixas de potenciais e valores de intensidade de tensão a partir dos quais ocorre o surgimento de trincas por C.S.T.. Fêz-se análises metalográficas dos corpos-de-prova onde se pode constatar trincas transgranulares bem típicas do fenômeno de C.S.T.. Foram feitos alguns testes em solução aquosa saturada de MgCl2, em ebulição, para se comparar as diferentes soluções quanto ao fenômeno de C.S.T.. Alterou-se as dimensões do corpo-de-prova para avaliar a orientação da propagação das trincas por C.S.T..

Nitretação a plasma do aço ABNT 316L em baixas temperaturas

A nitretação dos aços inoxidáveis austeníticos apresenta grande interesse tecnológico, pois tanto em processos convencionais tais como as nitretações a gás e em banho de sais como em processos a plasma, obtêm-se um aumento significativo de sua dureza superficial e resistência ao desgaste. No entanto, devido as altas temperaturas utilizadas nos processos convencionais, observa-se uma extensa formação de precipitados de nitretos de cromo, com consequente redução de resistência à corrosão do material. A proposta deste trabalho é utilizar a tecnologia de plasma para nitretar um aço inoxidável austenítico neste caso o ABNT 316 L a temperaturas relativamente baixas a fim de evitar precipitação de nitretos). As temperaturas utilizadas foram de 350, 375 e 400 0C, variandose o tempo de nitretação de 3 ,4 e 5 horas com duas misturas gasosas (76%N2 e 24%H2 e 5%H2 e 95%N2). As amostras foram analisadas através da microdureza superficial (método convencional e nanodureza), caracterização microestrutural por microscopia ótica, eletrônica de varredura e de transmissão, medida da profundidade de camadas formadas (MEV), rugosidade, determinação das fases presentes (Raios - X), nanodureza , perfil da composição química (GDOS) e resistência à corrosão (névoa salina e curvas de polarização) As amostras nitretadas nestas temperaturas e tempos produziram camadas de 1,9 a 5,5 µm medidas via GDOS e durezas que vão de 330HK a 987HK não observando-se a precipitação de nitretos de cromo, mas sim a formação de uma estrutura supersaturada de nitrogênio intersticial, chamada de “fase S” identificada por difração de Raios - X. As camadas nitretadas apresentaram um gradiente de nitrogênio que diminui, indicando um gradiente junto as características microestruturais, níveis de tensões residuais favoráveis para uma boa adesão, com a formação de uma camada com menor fragilidade. Esta fase “S”, além de produzir altas durezas superficiais, aumentou a resistência à corrosão do aço. Testes em campo com navalhas de corte e facas móveis tiveram um aumento de vida útil de 100% e 217%.