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原位漫反射红外光谱中采用新的实验手段研究煤岩显微组分中的氢键 总被引:4,自引:0,他引:4
首次提出采用小瓷片反应器,结合增大载气流量的方法进行产生挥发组分固体的原位漫反射红外光谱实验,研究了两种煤的镜质组和丝质组中的氢键分布及热稳定性.两种显微组分间氢键分布的规律相似;镜质组中SH-N、羧酸二聚体和自缔合羟基等的热稳定性比丝质组中的高.但对OH-N、羟基四聚体和OH-OR2的热稳定性随煤岩组分的变化无明显规律;随着温度的升高,OH-π含量先升高后降低,于350~380℃达最大值,其中镜质组OH-π的含量增加较快.显微组分中氢键的变化规律反映了其结构上的差异. 相似文献
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褐煤中水分的原位漫反射红外光谱研究 总被引:5,自引:0,他引:5
采用漫反射红外光谱(DRIFT)法,以140℃时褐煤的单光束图为背景研究了两种褐煤中的水分.结果表明,褐煤中水分的含量与光谱图相应区域的积分面积呈线性关系;在计算煤中水分形成的氢键键能的基础上,讨论了水分与煤表面间的氢键相互作用;根据DRIFT谱,将煤中的水分分为游离态的水与以弱氢键与煤表面结合的水和与煤形成强氢键的水.低于80℃时主要脱除前者,而高于80℃则主要脱除后者. 相似文献
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原位漫反射红外光谱技术用于气固催化反应机理的研究 总被引:1,自引:0,他引:1
漫反射傅立叶变换红外光谱技术是一种对固体粉末样品进行直接测量的光谱方法,是近年来发展起来的一项较理想的原位表征技术。原位漫反射红外技术由于可直接对催化剂表面的吸附态物种给出红外信号,可方便地跟踪鉴定反应中间态和产物,从而为催化反应体系反应机理的考察给出直接的证据。本文对于原位漫反射红外技术用于低温水煤气变换反应和水汽逆变换反应、醇类的水蒸汽重整、含CO2的合成气制取甲醇、低碳烃制合成气、CO催化氧化以及其他烃类和含氧化合物的氧化等方面进行了综述,认为该技术可很好地剖析气固相催化反应机理。 相似文献
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采用原位漫反射红外光谱法研究了Cuβ催化剂上氧化羰基合成碳酸二甲酯(DMC)的反应机理,考察了甲醇、一氧化碳和DMC的单独吸附及混合气吸附。结果表明,Cuβ催化剂上只存在一种活性位,位于六元环中;氧气能够氧化吸附态的甲醇产生甲氧基和水;DMC吸附在Cuβ催化剂上时,以羰基中的氧原子吸附在活性位上更加稳定;反应存在生成单甲氧基物种和双甲氧基物种两条路径,单甲氧基物种与CO反应生成单甲基碳酸盐物种(MMC),MMC再与甲氧基反应生成DMC;CO插入双甲氧基物种也可以得到DMC。在Cuβ催化剂上更倾向于进行CO插入双甲氧基物种这一路径。 相似文献
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温和条件下甲醛在 Pt/TiO2 上催化氧化反应的原位漫反射红外光谱研究 总被引:1,自引:0,他引:1
采用原位漫反射红外光谱研究了温和条件下 1%Pt/TiO2 催化剂上甲醛的吸附和氧化反应, 并对催化剂的失活进行了分析. 结果表明, Pt/TiO2 催化剂在室温条件下即可将甲醛氧化成 H2O 和 CO2, 100 oC 以下甲酸根的分解为决速步骤, 低温下催化剂失活是由于表面未能及时分解的甲酸根占据了催化剂的活性位, 升温至 100 oC 即可将甲酸根完全分解并恢复催化剂的活性. 相似文献
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以红外光谱法研究了丙烯酸聚醚聚氨酯合成反应(其中有氢键效应存在)及其反应动力学。结果表明:由于丙烯酸聚氨酯分子链结构中含有-CO-O-;-NH-和-O-三种主要极性基因,导致在反应中存在明显的氢键变化。在第一步聚氨酯预聚体合成中,氢键距离R随反应进行而逐渐减小,反映出-NHCO-O-结构增加,聚集加强,氢键作用加强,并趋向稳定;其中不同结构聚氨酯预聚体氢键距离R不同:R_(MDI)>R_(HDI)>R_(TDP),链段结构中有序程度依次降低。在第二步丙烯酸聚氨酯合成中,存在明显键效应,其链段结构中有序程度较原来预聚体稳定或略有下降。在二步合成反应过程中,1/1-P_(NCO)和t之间呈现很好的线性关系,表明这两步合成均属二级反学动力学。其区别在于第一步反应速率常数(k_1)较第二步反应速率常数(k_2)小一个数量级。 相似文献
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采用原位漫反射红外光谱法研究高温高压下CO H2在Rh-Mn-Li/SiO2催化剂上合成乙醇的反应中间体和反应机理,结果显示:2 922 cm-1,2855 cm-1两峰主要是由乙醇合成前体卡宾H2C=M的振动造成的;250℃,3.4 MPa时卡宾能在催化剂表面快速大量形成,反应后吹扫实验显示卡宾在催化剂表面的吸附并不相同,部分吸附较弱易脱附;部分吸附较强,在催化剂表面以相当稳定的形态存在,难以脱附;因此可能存在部分惰性卡宾,其不参与反应却占据了催化剂的部分表面,降低了催化剂的反应活性.250℃时,压力从0.5 MPa升高到3.0 MPa时,产物中CO2和CH4的含量降低,而乙醇的含量增加;反映出压力是影响反应产物分布的重要因素,压力提高能增大乙醇在产物中含量;同时也揭示出在该催化剂上CO2、CH4的生成路径与乙醇的生成路径存在着竞争性,压力是影响反应路径选择的重要因素.实验结果还表明卡宾的形成不是合成乙醇的速控步骤,而乙酰基能否大量形成则决定着乙醇产生的快慢.经过红外光谱分析后认为"CO缔合-卡宾-乙烯酮-乙酰基-乙醇"应是Rh基催化剂上合成乙醇较为合理的机理. 相似文献
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Michael Falk 《Mikrochimica acta》1988,94(1-6):203-205
OH stretching fundamentals in the spectra of hydrogen-bonded crystals are accompanied by satellite bands due to sum and difference transitions involving one quantum of the OH stretching vibration and one or more quanta of the low-frequency vibration of the hydrogen bond. Such satellites were detected in the FT-IR spectra of two hydrogen-bonded crystals, ice and methanol.NRCC No. 29006 相似文献
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Herein a well-sealed and thermostated kinetics assembly is designed and built, which can run stirred at different reaction temperatures. With the reaction assembly above and the volumetric method together, the hydrogen peroxide (H2O2) decomposition reaction kinetics is systematically investigated under a variety of reaction conditions over a copper-doped buserite-type layer manganese oxide (referred to as Cu-buserite) as a heterogeneous catalyst. The overall second-order rate law is fitted out by the linear regression analysis, with the reaction orders with respect to both H2O2 and Cu-buserite determined to each be equal to 1, and then explicitly explained by the proposed Michaelis-Menten like mechanism. The apparent activation energy Ea is estimated as 33.5 ± 2.5 kJ mol−1. 相似文献
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Geometrical parameters associated with N-H ... N types of hydrogen bonds have been analysed using crystal structure data on
nucleic acids, amino acids and related compounds. Histograms depicting the frequency distribution of N-H ... N length (l) and H-N ... N angle (θ) have been drawn and conclusions on the favoured geometry of such bonds have been arrived at. The
distribution ofl shows a pronounced maximum in the range between 2.9? and 3.0? with an overall average of 2.98 ?. The θ distribution shows
a pronounced maximum for the hydrogen bond angle in the range 0°-10°, with a rapid fall-off in frequency for nonlinear hydrogen
bonds. The frequency shows a cos6θ dependence as compared to cos2θ dependence term used earlier to predict the angular dependence of hydrogen bond potential energy in proteins and polypeptides. 相似文献
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Hydrogen bonds are very common and important interactions in biological systems, they are used to control the microenvironment around metal centers. It is a challenge to develop appropriate models for studying hydrogen bonds. We have synthesized two metal complexes of the phenol-tailed porphyrin, [Zn(HL)] and [Fe(HL)(C6H4(OH)(O))]. X-ray crystallography reveals that the porphyrin functions as a dianion HL2? and the phenol OH is involved in hydrogen bonds in both structures. In [Zn(HL)], an intramolecular hydrogen bond is formed between the carbonyl oxygen and OH. In [Fe(HL)(C6H4(OH)(O))], the unligated O(5) of the ligand is involved in two hydrogen bonds, as a hydrogen bond donor and a hydrogen bond acceptor. The overall electronic effect on the ligand could be very small, with negligible impact on the structure and the spin state of iron(III). The structural differences caused by the hydrogen bonds are also discussed. 相似文献
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We have measured the Raman spectra of liquid methanol at temperatures between 50° and –77°C. The weak O–H stretching bands appear, under amplification, more and more asymmetric as the temperature is lowered. They can be decomposed into three Gaussian components centered at about 3220, 3310, and 3400 cm–1. The former, predominant at low temperature, corresponds to single, linear hydrogen bonds (LHB) between two molecules. The other two are assigned to branched hydrogen bonds, respectively bifurcated (BHB), between three molecules, and trifurcated (THB), between four molecules. We conclude that the molecular structure of liquid alcohols is not chain-like, as presumed so far, but a three-dimensional network featuring a mixture of single (LBH), and multiple hydrogen bonds (BHB, and THB). They are mainly electrostatic in nature, their relative proportions and geometry governed by the packing conditions for minimum energy. They form distinct trimers and tetramers in dilute solutions of alcohols in inert solvents and frozen matrices, and the latter even in the vapor.Deceased December 25, 1987. 相似文献
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The equilibrium structures, binding energies, and vibrational spectra of the complexes formed between hydrogen fluoride clusters (HF)n (1≤n≤4) and the fluorosilanes SiHF3, SiH2F2, and SiH3F are investigated within the second-order Møller–Plesset perturbation theory method applying extended basis sets. It is shown that Si–FH–F halogen–hydrogen bonds are formed in the most stable open dimers, SiHF3–HF, SiH2F2HF, and SiH3FHF. No Si–HF–H hydrogen bonds occur in these dimers. Nevertheless, blue shifts of Si–H stretching frequencies are calculated. All three trimers, fluorosilane–(HF)2, all three tetramers, fluorosilane–(HF)3, and two of the pentamers, fluorosilane–(HF)4, form cyclic structures with strong Si–FH–F halogen–hydrogen bonds and weak Si–HF–H contacts, the latter displaying, nevertheless, strongly blue-shifted Si–H stretching frequencies. These blue shifts are comparable in size to those of the corresponding fluoromethane–(HF)n complexes and are with about +50 cm−1 for the case n=3 among the largest ever calculated and definitely the largest for Si–H bonds. In the title complexes, the formation of the Si–FH–F halogen–hydrogen bonds induces a substantial stretching of this Si–F bond, which in turn leads to a significant contraction of the fluorosilane Si–H bond in the Si–HF–H hydrogen bond. This disposition of the fluorosilane monomers is demonstrated with the aid of suitable potential energy surface scans and appears to be a prerequisite for the formation of strongly blue-shifted hydrogen bonds. 相似文献
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A method for the identification of hydrogen bonds was investigated from the viewpoint of the stress tensor density proposed by Tachibana and following other works in this field. Hydrogen bonds are known to exhibit common features with ionic and covalent bonds. In quantum electrodynamics, the covalent bond has been demonstrated to display a spindle structure of the stress tensor density. Importantly, this spindle structure is also seen in the hydrogen bond, although the covalency is considerably weaker than in a typical covalent bond. Distinguishing it from the ionic bond is most imperative for the identification of the hydrogen bond. In the present study, the directionality of the hydrogen bond is investigated as the ionic bond is nearly isotropic, while the hydrogen bond exhibits the directionality. It was demonstrated that the hydrogen bond can be distinguished from the ionic bond using the angle dependence of the largest eigenvalue of the stress tensor density. 相似文献
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氢能作为一种理想的二次能源受到了国内外科研工作者的广泛关注,研制可以在室温和较低压力下方便、安全、高效地储存氢能的材料是氢能发展的瓶颈.到目前为止,固态储氢材料以能量密度高及安全性好等优势被认为极具应用前景,其中以轻质元素构成的氢化物(包括硼氢化物/铝氢化物(可用通式A(MH4)n表示,其中A是碱金属(Li,Na,K)或碱土金属(Be,Mg,Ca);M是硼或铝;n=1~4)、氨基氢化物(如LiNH2等))、氨硼烷(NH3BH3)、金属有机骨架材料(MOFs)是新型储氢材料研究领域的热点,本文将着重就目前这几类储氢材料的研究当中所涉及到的一些热力学及动力学问题进行总结探讨. 相似文献