不同金属改性对Pt/β-分子筛催化柴油车尾气中HC、CO及SO_2氧化性能的影响

采用共浸渍法制备了Ce、Cr、Mo和Cu改性的Pt/β-分子筛催化剂,运用氮吸附、XRD、H_2-TPR、NH_3-TPD和XPS等手段对该催化剂进行了表征,研究了不同金属改性对催化剂的织构性质、骨架结构、表面酸性以及在模拟柴油车尾气中抑制SO_2氧化性能和催化HC、CO氧化活性的影响。结果表明,金属改性对催化剂织构性能和骨架结构影响较小。Cr、Mo和Cu的添加可以调变催化剂酸强度,进而抑制SO_2的氧化;Cu改性的催化剂具有最好的抑制SO_2氧化的能力,在350和450℃条件下,与未改性Pt/β-分子筛催化剂相比,Cu改性催化剂上SO_2转化率分别下降了70.4%和70.2%。然而,改性金属与Pt物种之间产生的相互作用,会使Pt物种更难还原,导致Pt对HC和CO氧化的催化活性降低。     

REUSY-Ex的吸附性能及二次孔结构研究

应用高真空重量法(分别以苯和正庚烷为吸附质)和低温N2吸附法对REUSY-Ex的吸附性能和二次孔结构进行了研究.结果表明,在水热处理过程中可产生二次孔结构,且二次孔的形成与水热处理的脱铝深度相关.稀HCl浸取REUSY不仅能浸取出位于其二次孔中的非骨架铝(EFAL)碎片,而且还能浸取出位于微孔中的EFAL。29Si MAS NMR的结果显示,稀HCl浸取后,骨架Si(OAl)的谱宽变窄,裂分效果提高,表明其化学环境单一或均匀.     

HFC/HC混合工质共沸点的推算

HFC/HC混合工质的气液性平衡实验研究结果表明,该类型混合工质大多存在共沸现象。根据形成共沸点的热力学条件,以PR状态方程结合vdW混合法则,利用建立的二元相互作用系数k_ij差值关联模型,对10种HFCs工质（HFC23、HFC32、HFC125、HFC143a、HFC134a、HFC152a、HFC227ea、HFC236fa、HFC236ea、HFC245fa）与3种HCs工质（HC290、HC600a、HC600）相互组合而成的30种HFC/HC混合工质进行了共沸点判断和共沸点性质推算,并与已有气液相平衡实验数据的体系进行对比。结果表明该方法可用于推算HFC/HC混合工质共沸点性质。     

Development of an Extractive Continuous Monitor For Hydrogen Chloride (Hc1) Analyses of Coal-Derived Process Streams

Abstract

An HC1 monitor has been developed at the Morgantown Energy Technology Center (METC) for the extractive analysis of hightemperature/high-pressure, coal-derived process streams. This monitor is capable of HC1 concentration measurement in the presence of all known coal gasification products. Detection is based on the ability of HC1 to protonate a high boiling alcohol (solvent) and, thus, enhance the conductivity of the alcohol. Conductivity is then related to HC1 concentration. the observed high degree of sensitivity that can be achieved is a result of analyte preconcentration prior to the conductivity measurement due to the apparently fast dissolution rate of HC1 into the alcohol solvent coupled with a large analyte gas-to-solvent ratio. the linear dynamic range of the HC1 monitor is two orders of magnitude. However, since the degree of preconcentration can be adjusted by changing either the solvent or analyte gas flow rate, the HC1 monitor has an extended operating range of six orders of magnitude (ppb lower limit, percentage upper limit). the practical lower detection limit for the HC1 monitor is estimated to be 50 ppbv. Precision is good with typical relative average deviations of about three parts per hundred. Although the HC1 monitoring method was originally designed for the analysis of gasification process streams, the system can be adapted for use with a variety of process gas streams.     

Is the DPT tautomerization of the long A·G Watson–Crick DNA base mispair a source of the adenine and guanine mutagenic tautomers? A QM and QTAIM response to the biologically important question

Herein, we first address the question posed in the title by establishing the tautomerization trajectory via the double proton transfer of the adenine·guanine (A·G) DNA base mispair formed by the canonical tautomers of the A and G bases into the A*·G* DNA base mispair, involving mutagenic tautomers, with the use of the quantum‐mechanical calculations and quantum theory of atoms in molecules (QTAIM). It was detected that the A·G ? A*·G* tautomerization proceeds through the asynchronous concerted mechanism. It was revealed that the A·G base mispair is stabilized by the N6H···O6 (5.68) and N1H···N1 (6.51) hydrogen bonds (H‐bonds) and the N2H···HC2 dihydrogen bond (DH‐bond) (0.68 kcal·mol^?1), whereas the A*·G* base mispair—by the O6H···N6 (10.88), N1H···N1 (7.01) and C2H···N2 H‐bonds (0.42 kcal·mol^?1). The N2H···HC2 DH‐bond smoothly and without bifurcation transforms into the C2H···N2 H‐bond at the IRC = ?10.07 Bohr in the course of the A·G ? A*·G* tautomerization. Using the sweeps of the energies of the intermolecular H‐bonds, it was observed that the N6H···O6 H‐bond is anticooperative to the two others—N1H···N1 and N2H···HC2 in the A·G base mispair, while the latters are significantly cooperative, mutually strengthening each other. In opposite, all three O6H···N6, N1H···N1, and C2H···N2 H‐bonds are cooperative in the A*·G* base mispair. All in all, we established the dynamical instability of the А*·G* base mispair with a short lifetime (4.83·10^?14 s), enabling it not to be deemed feasible source of the A* and G* mutagenic tautomers of the DNA bases. The small lifetime of the А*·G* base mispair is predetermined by the negative value of the Gibbs free energy for the A*·G* → A·G transition. Moreover, all of the six low‐frequency intermolecular vibrations cannot develop during this lifetime that additionally confirms the aforementioned results. Thus, the A*·G* base mispair cannot be considered as a source of the mutagenic tautomers of the DNA bases, as the A·G base mispair dissociates during DNA replication exceptionally into the A and G monomers in the canonical tautomeric form. © 2013 Wiley Periodicals, Inc.     

高效液相色谱法同时测定染发剂中8种合成染料

使用甲醇对样品进行超声提取,以乙腈-0.02 mol/L乙酸铵溶液为流动相,采用XB-C18色谱柱分离,二极管阵列检测器检测,外标法定量,建立了同时测定染发剂中8种合成染料的高效液相色谱分析方法。HC红3号、分散黑9、HC黄2号、分散紫1及HC橙1号的检测波长设为240 nm,HC黄4号设为410nm,HC蓝7号为450 nm,HC红1号为270 nm。8种染料在0.5~100.0μg/m L范围内具有良好线性,相关系数(r2)均不小于0.999 3。HC红3号、HC黄4号、HC橙1号和分散紫1的检出限均为0.70 mg/kg,分散黑9、HC黄2号、HC蓝7号和HC红1号的检出限分别为2.50,0.60,0.35,0.50 mg/kg。样品的平均回收率为85.4%~99.8%,相对标准偏差(n=6)为1.1%~3.6%。方法的精密度、准确度、回收率和基质效应均符合染发剂样品测定的要求,用于实际样品测定,结果满意。该方法快速简便、定量准确,能满足染发剂中8种合成染料含量的分析检测要求。     

空调循环中HCs/阻燃剂混合工质的泄漏特性

结合空调循环分析了非共沸HCs/阻燃剂混合工质的泄漏特性,包括一定泄漏率下引起最大组成变化的泄漏点和工质相态、泄漏率-总组成变化关系、泄漏引起的组成变化对HCs/阻燃剂混合工质安全性与循环性能的影响分析。     

Pilot-plant for NOx, SO2 and HC removal from flue-gas of municipal waste incinerator by electron beam irradiation

According to the basic research performed using a small size reactor at TRCRE of JAERI, the electron beam irradiation process was proved to be very effective for NO_x, SO₂ and HC removals from flue-gas of municipal waste incinerators. Based on this result, a pilot-plant was constructed for the demonstration of NO_x, SO₂ and HC removal performance using electron accelerator of maximum energy 0.95 MeV and maximum power 15kW.The pilot-plant was constructed at Matsudo City waste Disposal Center. The flue-gas of 1,000 Nm³/hr is guided from the waste incinerator flue-gas line of 30,000Nm³/hr to the pilot-plant to be processed by spraying Ca(OH)₂ slurry or powder and irradiation with high-energy electron beam of the accelerator. NO_x, SO₂ and HC are removed simultaneously from the flue-gas by the enhanced reaction with Ca (OH)₂ under irradiation.A brief explanation of the pilot-plant and preliminary results of the experiments are introduced in this paper.     

Crystal structure of 1,3-diphenyladamantane and trans-1,4-diphenylcyclohexane: torsion angles about C-Ph bonds in α,ω-diphenyl(alicyclic hydrocarbon)

The orientation of the two phenyl rings in α,ω-diphenylalkanes with rigid carbon skeletons is investigated through characterization of the crystal and molecular structures of 1,3-diphenyladamantane (1) and trans-1,4-diphenylcyclohexane (2). The two phenyl rings in 1 have different conformations about the C-Ph bonds, with torsion angles between the phenyl ring and the C1-C2-C3 plane of 0.65 and 71.7°. A hydrogen atom at the meta-position of one of the phenyl rings contact intermolecularly with a tertiary hydrogen atom at C5 of adamantane within the sum of van der Waals radii. Due to the helical conformation, the short CH?HC contacts (2.231 Å) construct supramolecular triple helical strands. In contrast to 1, the phenyl rings in 2 have identical configurations, with equatorial position and bisected conformation as expected from density functional calculations. The molecular packing of 2 exhibits a herringbone pattern of (aromatic)C-H?π contacts.     

Linear and nonlinear feature of electronic excitation energy in carbon chains HC2n+1H and HC2nH

Density functional theory has been used to investigate the geometries, bonding, and vibrational frequencies of HC_2nH (n = 1–13) and HC_2n+1H (n = 2–12). Vertical excitation energies for the X¹Σ → 1¹Σ transition of HC_2nH (n = 1–5) and for the X³Σ → 1³Σ transition of HC_2n+1H (n = 2–5) have been calculated by the time‐dependent density functional theory and ab initio second‐order multiconfiguration perturbation method, respectively. On the basis of the present calculations, explicit expressions for the size dependence of excitation energy in linear polyynes HC_2n+1H and HC_2n+1H are suggested. Such analytical λ ? n relationships show good agreement with experimental observations. Theoretical investigations of relevant excited states demonstrate that distinct linear and nonlinear spectroscopic features in such polyynes can be ascribed to similarity and difference in bonding between the ground and excited states in HC_2n+1H and HC_2nH. © 2004 Wiley Periodicals, Inc. Int J Quantum Chem, 2004