氩吸附法研究多级孔分子筛的孔结构

采用不同方法分别制备了双介孔分子筛、介微孔分子筛及介孔沸石材料,利用氩吸附法并结合XRD技术表征了多级孔分子筛的孔结构。探讨了适用于多级孔分子筛的孔径分布计算方法,揭示了不同类型吸附等温线与孔径分布、孔型及孔容等之间的关系。研究表明,对于多级孔分子筛、微孔和介孔的孔径分布分别用SF法和BJH法计算较适宜,全孔分析可用NLDFT法计算。通过对TS-1介孔沸石的孔结构分析发现, TPAOH 在改性制备介孔TS-1的过程中起到了生成介孔及促进二次晶化的双重作用。     

活性炭孔隙结构对催化氧化脱除单质汞的影响

研究活性炭在硫化氢存在条件下催化氧化脱除煤气中单质汞的吸附机理和探讨提高其吸附能力的方法,在模拟煤气气氛下对3种活性炭和一种活性焦进行汞的吸附性能实验,并进一步分析活性炭(焦)的孔隙结构。用BET方程处理N₂等温吸附数据,计算比表面积;用HK法进行微孔分析;用BJH法计算中孔孔径分布。结果表明,硫化氢被催化氧化后,生成吸附在活性炭孔壁上的活性硫促进了对汞的吸附;随着活性炭微孔和中孔体积的增大,活性炭对汞的吸附能力得到提高。     

多孔活性炭孔径分布的表征

总结了利用气体吸附法表征多孔活性炭中孔和微孔孔径分布的各种方法。BJH方法和MP模型忽略了微孔内势能叠加效应,仅适合描述中孔孔径分布;HK模型和以Dubinin填充理论为基础的各种方法,考虑了微观下势能叠加的效果,在一定程度上能很好地描述微孔孔径分布;最近围绕GAI(GeneralizedAdsorptionIsotherm)而展开的利用密度范函理论(DFT,densityfunctiontheory)和巨正则系综蒙特卡罗(GCMC,grandcanonicalensemblemontecarlo)模拟确定微孔孔径分布的方法较好地克服了Dubinin理论中存在的缺点,是较好的两种方法,但其有效性还需要更多的实验结果来证明。     

比表面积与孔径分布测定及计算中一些问题的研究Ⅲ.关于微孔法孔结构分析

本文对孔结构分析的微孔法(简称MP法)及其理论基础v-t曲线进行了分析研究,指出deBoer等对v-t曲线的三种分类不是三种机理的充分必要条件,从准确性看,基于填充机理的MP法并不比基于凝聚机理的方法好,而是各有优点.     

用CO_2吸附法分析分子筛的孔结构

以NaA,NaY和NaZSM-5分子筛为研究对象,以CO2为吸附质,通过吸附数据测定,研究分子筛材料微孔结构的吸附表征方法.计算了NaA、NaY和NaZSM-5分子筛的微孔孔容,其中基于D-A方程的微孔孔容值与文献值一致.根据CO2吸附数据分析了3种分子筛的孔径分布.发现对于含有球形孔结构的NaA,NaY分子筛和NaA+NaY混合物,HK(Horvath-Kawazoe)球形模型(HKsphere)能够很好地描述其孔径分布,而HK柱状模型(HKcylinder)能够很好地表征具有柱状孔道结构的NaZSM-5分子筛.单一的HK方法不能表征同时含有柱状孔和球形孔的NaA+NaZSM-5混合物,使用HKcylinder只能得到混合物材料中柱状孔的分布情况,而使用HKsphere只能得到球形孔的分布情况.     

几种植物基活性炭材料的孔结构与吸附性能比较——(I)孔结构表征

测定了3种植物基活性炭材料:椰壳活性炭 (CAC4)、剑麻茎基活性炭 (SSAC) 和剑麻基活性碳纤维 (SACF) 的氮吸附等温线,并用不同的理论方法对其孔结构进行了分析和表征。结果表明:CAC4为微孔型,孔径分布集中且大部分是0.7nm以下的极微孔;在相同条件下制备的SSAC和SACF孔分布较为相似,都呈多分散性,结构中除微孔外,还含有丰富的中孔,中孔率均超过50%以上。两者相比,SACF的中孔量和平均孔径更大。3个样品的形态特征和孔结构虽然不同,但其吸附过程都可以用微孔多段填充机理来解析。     

对微孔吸附常用经典分析模型的比较

文章采用列表对比的方式,简要介绍了微孔吸附常用经典模型的出处、应用范围、发展历史和各自的特点。为了方便系统了解和掌握物理吸附中的微孔经典分析方法,文章将其分成三类：(1)由标准等温线发展出的方法,包括t-图法、αs-图法、n-图法和MP法;(2)基于微孔填充理论的方法,包括D-R方法、D-A方法和D-R-S方法;(3)目前普遍使用的方法,包括原始HK方法(狭缝型孔)、HK-SF方法(圆柱型孔)和HK-CY方法(球型孔)以及三种改进后的HK方法。     

几种植物基活性炭材料的孔结构与吸附性能比较--(Ⅰ)孔结构表征

测定了3种植物基活性炭材料：椰壳活性炭(CAC4)、剑麻茎基活性炭(SSAC)和剑麻基活性碳纤维(SACF)的氮吸附等温线，并用不同的理论方法对其孔结构进行了分析和表征．结果表明：CAC4为微孔型，孔径分布集中且大部分是0．7nm以下的板微孔：在相同条件下制备的SSAC和SACF孔分布较为相似，都呈多分散性，结构中除微孔外，还含有丰富的中孔，中孔率均超过50％以上．两者相比，SACF的中孔量和平均孔径更大，3个样品的形态特征和孔结构虽然不同，但其吸附过程都可以用微孔多段填充机理来解析。     

聚二乙烯苯型多孔吸附剂的纳米孔结构表征

采用氮气吸附法 ,研究聚二乙烯苯多孔吸附剂的纳米孔结构 .结果表明 ,以甲苯 液体石蜡 (2 :1)为致孔剂制备的聚二乙烯苯多孔吸附剂 ,其比表面和孔体积随致孔剂用量增大而增加 .在二乙烯苯总含量相当时 ,m 二乙烯苯与p 二乙烯苯等比例混合制备的吸附剂 ,具有最大的比表面和孔体积 ,而聚m 二乙烯苯吸附剂和聚p 二乙烯苯吸附剂依次下降 .中孔分布研究说明 ,各种吸附剂的中孔主要分布在 2～ 2 0nm之间 ,其中在5nm附近存在一个明显的分布峰 ,是吸附剂在制备时由于致孔剂的存在而在微核 微核之间形成的孔 .微孔分布研究发现 ,聚m 二乙烯苯吸附剂和聚p 二乙烯苯吸附剂的微孔集中分布在 0 .4～ 1.2nm之间 ,这些微孔可能是微核内部不规整聚集的高分子链之间的缝隙和紧密接触的微核之间的缝隙 .用扫描电镜观察吸附剂内部 ,显示吸附剂的确是由微核聚集形成的 ,其间存在着大小不同的纳米尺度的空隙     

聚丙烯腈基碳纤维及其原丝中的微孔尺寸分布

利用二维小角X射线散射技术(SAXS)研究了聚丙烯腈基碳纤维及其原丝的微孔结构。结合逐级切线法、对数正态分布及麦克斯韦分布函数对2类实验样品内部微孔的尺寸分布进行了分析。结果表明,2类样品中的孔结构具有显著差别,原丝微孔在4~8 nm范围内分布比较集中,碳纤维中微孔的分布区域则移向1.3~1.8 nm。散射数据显示出明显的分形特征,碳纤维与其原丝的孔分形维数分别为1.33和1.55,表明原丝中具有较大的孔隙缺陷。相对于原丝,碳纤维微孔尺寸分布走向均匀和集中,前者则表现出比后者更宽的尺寸分布。就拟合方法而言,逐级切线法的解析手段容易引入误差,低角区的纤维表面散射和高角区的噪音容易对其结果造成影响。正态分布得到了比较窄的尺寸分布,但对于低尺寸区域孔隙的拟合不理想。麦氏分布在一定程度上弥补了以上不足,能够较好地拟合两类纤维样品中微孔的分布状况。     

The effective fragment potential: small clusters and radial distribution functions

The effective fragment potential (EFP) method for treating solvent effects provides relative energies and structures that are in excellent agreement with the analogous fully quantum [i.e., Hartree-Fock (HF), density functional theory (DFT), and second order perturbation theory (MP2)] results for small water clusters. The ability of the method to predict bulk water properties with a comparable accuracy is assessed by performing EFP molecular dynamics simulations. The resulting radial distribution functions (RDF) suggest that as the underlying quantum method is improved from HF to DFT to MP2, the agreement with the experimental RDF also improves. The MP2-based EFP method yields a RDF that is in excellent agreement with experiment.     

Improved third-order Møller-Plesset perturbation theory

Based on a partitioning of the total correlation energy into contributions from parallel‐ and antiparallel‐spin pairs of electrons, a modified third‐order Møller–Plesset (MP) perturbation theory is developed. The method, termed SCS–MP3 (SCS for spin‐component‐scaled) continues previous work on an improved version of MP2 (S. Grimme, J Chem Phys 2003, 118, 9095). A benchmark set of 32 isogyric reaction energies, 11 atomization energies, and 11 stretched geometries is used to assess to performance of the model in comparison to the standard quantum chemical approaches MP2, MP3, and QCISD(T). It is found, that the new method performs significantly better than usual MP2/MP3 and even outperforms the more costly QCISD method. Opposite to the usual MP series, the SCS third‐order correction uniformly improves the results. Dramatic enhancements are especially observed for the more difficult atomization energies, some of the stretched geometries, and reaction and ionization energies involving transition metal compounds where the method seems to be competitive or even superior to the widely used density functional approaches. Further tests performed for other complex systems (biradicals, C₂₀ isomers, transition states) demonstrate that the SCS–MP3 model yields often results of QCISD(T) accuracy. The uniformity with which the new approach improves for very different correlation problems indicates significant robustness, and suggests it as a valuable quantum chemical method of general use. © 2003 Wiley Periodicals, Inc. J Comput Chem 24: 1529–1537, 2003     

Scaled opposite-spin second order Møller-Plesset correlation energy: an economical electronic structure method

A simplified approach to treating the electron correlation energy is suggested in which only the alpha-beta component of the second order M?ller-Plesset energy is evaluated, and then scaled by an empirical factor which is suggested to be 1.3. This scaled opposite-spin second order energy (SOS-MP2), where MP2 is M?ller-Plesset theory, yields results for relative energies and derivative properties that are statistically improved over the conventional MP2 method. Furthermore, the SOS-MP2 energy can be evaluated without the fifth order computational steps associated with MP2 theory, even without exploiting any spatial locality. A fourth order algorithm is given for evaluating the opposite spin MP2 energy using auxiliary basis expansions, and a Laplace approach, and timing comparisons are given.     

Highly‐Sensitive Determination of 6‐Mercaptopurine and Its Metabolites by Electrochemical Reductive Desorption Measurements

The electrochemical detection of 6‐mercaputopurine (6‐MP), which is one of the most well‐known drugs of antimetabolites, and its analogues was studied. The presented method is based on chemisorption (accumulation)/desorption processes of drugs onto/from the Au electrode surface. Using this method, we succeeded in detecting 6‐MP even in very diluted solution (concentration of 6‐MP: 1×10^?8 M). The lower detection limit of 6‐MP was considerably improved compared with the previous HPLC studies by using our proposed system. Desorptive potentials of 6‐MP‐metabolites and its analogues were different from those of 6‐MP. This provides the possibility of simultaneous detection of 6‐MP and its typical metabolites.     

Hybrid correlation models based on active-space partitioning: seeking accurate O(N5) ab initio methods for bond breaking

Moller-Plesset second-order (MP2) perturbation theory remains the least expensive standard ab initio method that includes electron correlation, scaling as O(N5) with the number of molecular orbitals N. Unfortunately, when restricted Hartree-Fock orbitals are employed, the potential energy curves calculated with this method are of little use at large interatomic separations because of the divergent behavior of MP2 in these regions. In our previous study [J. Chem. Phys. 122, 234110 (2005)] we combined the MP2 method with the singles and doubles coupled cluster (CCSD) method to produce a hybrid method that retains the computational scaling of MP2 and improves dramatically the shape of the MP2 curves. In this work we expand the hybrid methodology to several other schemes. We investigate a new, improved MP2-CCSD method as well as a few other O(N5) methods related to the Epstein-Nesbet pair correlation theory. Nonparallelity errors across the dissociation curve as well as several spectroscopic constants are computed for BH, HF, H2O, CH+, CH4, and Li2 molecules with the 6-31G* basis set and compared with the corresponding full configuration interaction results. We show that among the O(N5) methods considered, our new hybrid MP2-CCSD method is the most accurate and significantly outperforms MP2 not only at large interatomic separations, but also near equilibrium geometries.     

The permanent dipole moment of gas-phase para-amino benzoic acid revisited

The permanent dipole moment of para-amino benzoic acid has been calculated at various theoretical levels, including Hartree-Fock, second-order M?ller-Plesset perturbation (MP2), coupled cluster singles and doubles (CCSD), and triples corrections CCSD(T), and hybrid density functional theory at B3LYP level. It is found that the B3LYP method fails to provide correct results for the geometry and the permanent dipole moment. These results are significantly improved by MP2 calculations. Our best estimated dipole moments obtained at CCSD and CCSD(T) levels are in good agreement with experiment.     

Improved supermolecular second order Møller-Plesset intermolecular interaction energies using time-dependent density functional response theory

The supermolecular second order Moller-Plesset (MP2) intermolecular interaction energy is corrected by employing time-dependent density functional (TDDFT) response theory. This is done by replacing the uncoupled second order dispersion contribution contained in the supermolecular MP2 energy with the coupled dispersion energy obtained from the TDDFT approach. Preliminary results for the rare gas dimers He2, Ne2, and Ar2 and a few structures of the (HF)2 and (H2O)2 dimers show that the conventional MP2 interaction energies are considerably improved by this procedure if compared to coupled cluster singles doubles with perturbative triples [CCSD(T)] interaction energies. However, the quality of the interaction energies obtained in this way strongly depends on the exchange-correlation potential employed in the monomer calculations: It is shown that an exact exchange-only potential surprisingly often performs better than an asymptotically corrected hybrid exchange-correlation potential. Therefore the method proposed in this work is similar to the method by Cybulski and Lytle [J. Chem. Phys., 127, 141102 (2007)] which corrects the supermolecular MP2 energies with a scaled dispersion energy from time-dependent Hartree-Fock. The results in this work are also compared to the combination of density functional theory and intermolecular perturbation theory.     

Scaled opposite spin second order Møller-Plesset theory with improved physical description of long-range dispersion interactions

Separate scaling of the same-spin and opposite spin contributions to the second-order M?ller-Plesset energy can yield statistically improved performance for a variety of chemical problems. If only the opposite spin contribution is scaled, it is also possible to reduce the computational complexity from fifth order to fourth order in system size, with very little degradation of the results. However neither of these scaled MP2 energies recovers the full MP2 result for the dispersion energy of nonoverlapping systems. This deficiency is addressed in this work by using a distance-dependent scaling of the opposite spin correlation energy. The resulting method is compared against the previously proposed scaled MP2 methods on a range of problems involving both short and long-range interactions.     

Poly(dimethylsiloxane)/palygorskite composites: preparation,characterization, and properties

Poly(dimethylsiloxane) (PDMS) composites were prepared by simple blending process using palygorskite (PG) or modified palygorskite (MP). This study has been designed to determine the influences of PG or MP on the thermal stability and the mechanical properties of PDMS composites. The thermal stability of PG and MP were also studied by thermogravimetric analysis (TGA). The results showed that MP had the similar thermal stability to PG, and PG or MP not only increased the thermal stability but also improved the mechanical properties of PDMS composites. Meanwhile, compared with PG/PDMS composites, MP/PDMS composites had better thermal stability and mechanical properties owing to the better dispersion of MP into the matrix, the stronger chemical interfacial interaction between MP and the matrix. Copyright © 2010 John Wiley & Sons, Ltd.