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甲醇处理煤的微孔性质及反应性研究 总被引:2,自引:0,他引:2
在低于临界温度下,用甲醇处理了三种不同变质程度的煤,以研究其比表面积及微孔容积等表面特性的变化。结果表明,用甲醇处理后煤的微孔性质发生了较大变化,其变化的大小顺序是:沈北褐煤>大同烟煤>晋城无烟煤。随甲醇处理温度或干馏温度升高,煤及半焦的孔径均向小的方向偏移。煤的平均孔径为8.2—8.6A;半焦的平均孔径为6.3—7.5A。煤经甲醇处理后其半焦的反应性均比未处理的高。 相似文献
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用聚苯乙烯标样作为探针,对多种SEC柱的分离和扩展效应作同时的校准,扩展因子随探针分子量的增加而增大,增大的幅度与SEC填料的孔洞表面结构有关。大孔径多孔硅球的比表面积较低,孔洞表面比较平滑,溶质分子在孔洞中运动时阻碍粳少,高分子量聚苯乙烯(M?10~6)的扩展因子只比低分子量(M?10~3)的大2—3倍。交联聚苯乙烯型凝胶的比表面积较大,表面比较粗糙,高分子量探针的扩展因子要比低分子量的高出几十倍,显示溶质分子在孔洞中运动所受阻碍较大。后一现象可用有机交联凝胶永久性孔洞的骨架表面具有自由链端得到说明。 相似文献
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本工作测定了NaCl、KCl在CH_3OH与DMF及CH_3OH与DMSO全组成范围混合溶剂中的溶解度。实验温度分别是; 对NaCl:278、288、298、303、313 K, 对KCl:288、303、313 K。随着溶剂组成变化KCl和NaCl的溶解度曲线皆有一极大值。溶解度温度系数分别为正和负, 随着溶剂中CH_3OH组份的减少温度系数减小。根据实验结果, 计算得NaCl和KCl自甲醇至混合溶剂的转移自由能和熵。对离子在此混合物中的溶剂化、结构影响和盐的溶解倾向作了初步解释。 相似文献
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The attractive Interactions between typically hydrophobic molecules such as hexane or CCl4, and the repulsive Interactions between extremely hydrophilic molecules such as poly(ethylene oxide) (PEO), when immersed in water, as well as the interactions between these molecules and water, have been examined from a surface thermodynamic viewpoint, taking the changes in surface free energy into account, as a function of temperature. It was found that attractive hydrophobic Interactions are not, as vas generally believed up to now, invariably entropic. Hydrophobic Interactions can be mainly enthalpic or mainly entropic, or more or less equal mixtures of both, depending on each individual case; however, all hydrophobic interactions are polar (in the sense of Lewis acid-base) in nature. Repulsive hydrophilic interactions are enthalpic, and also polar in nature. The interaction between hydrophobic solutes and water is mainly enthalpic, and is apolar in nature. 相似文献
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End-tethered polymer chains usually adopt mushroomlike structures on the surface when their density is low. The behaviors of these surface-attached hemicoils are described by existing polymer theory. Dolan and Edwards derived the free energy of a single polymer chain confined between two planar surfaces. Their theory was used to approximate the steric interaction free energy, E, of two identical surfaces bearing polymers in the mushroom regime and to compare with experimental data obtained from surface force measurements. However, because of a mislabeled plot in the original paper, experimental force profiles did not seem to fit the free energy approximation satisfactorily. We have correctly relabeled the involved plot and derived a new simple expression for E. In order to verify this expression, we have performed experiments on PEG45 polymers incorporated in lipid bilayers using a surface force apparatus. The measured force profiles are in perfect agreement with the prediction. We show that such measurements can be used to determine the local density of grafted polymer with good precision. 相似文献
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A. W. De Groot D. E. Guinnup M. H. Thiel J. A. Cuculo 《Journal of Polymer Science.Polymer Physics》1991,29(5):557-563
This is the second part of a two–part study of the NH3NH4SCN cellulose solvent system. Quasielastic light scattering was used to determine the diffusion coefficients of cellulose in solution and the effective hydrodynamic radius of the dissolved molecules. Additionally, the system was studied using light microscopy to determine the minimum critical volume fraction or liquid crystal formation. Very little change was found in the diffusion coefficients with change in cellulose concentration indicating little interaction between the chains in solution. Values of 7.69 and 2.66 × 108 cm2/s were measured for samples having a degree of polymerization of 153 and 969. The value of the coefficient relating the hydrodynamic volume to the radius of gyration was found to be in the range of 0.33 to 0.53, indicating an extended coil conformation according to the Kirkwood-Riseman theory. The minimum critical volume fractions necessary for liquid crystal formation, υ2′ were 0.039, 0.038, and 0.048 for the three solvent compositions studied. The values calculated for υ2′ based on the measured persistence lengths were much larger than the predicted values, indicating strong deviation from theory or possible aggregation in the system. 相似文献
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A mathematical model was proposed (1) in a recently published paper in an attempt to represent the formation of microemulsion systems. However, the model fits microemulsion systems only up to certain critical dispersed phase volume, known as the percolation threshold. A single total free energy minimum corresponding to a stable system was found by the model for phase volumes below the percolation threshold. If the dispersed phase volume is further increased, the model predicts instability with no free energy minimum. However, experimental results (1,2) indicate percolation of microdroplets above the percolation threshold before the system eventually breaks down upon further increase of the phase volume. An extra free energy term from the interaction between microdroplets is introduced and incorporated into the model. This new model now predicts two free energy minima above the percolation threshold of the dispersed phase corresponding to polydispersity of the system. Further increase in dispersed phase volume will then cause the system to become unstable. 相似文献
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Vehkamäki H McGrath MJ Kurtén T Julin J Lehtinen KE Kulmala M 《The Journal of chemical physics》2012,136(9):094107
The critical cluster is the threshold size above which a cluster will be more likely to grow than to evaporate. In field and laboratory measurements of new particle formation, the number of molecules of a given species in the critical cluster is commonly taken to be the slope of the log-log plot of the formation rate versus the concentration of the species. This analysis is based on an approximate form of the first nucleation theorem, which is derived with the assumption that there are no minima in the free energy surface prior to the maximum at the critical size. However, many atmospherically relevant systems are likely to exhibit such minima, for example, ions surrounded by condensable vapour molecules or certain combinations of acids and bases. We have solved numerically the birth-death equations for both an electrically neutral one-component model system with a local minimum at pre-critical sizes and an ion-induced case. For the ion-induced case, it is verified that the log-log slope of the nucleation rate versus particle concentration plot gives accurately the difference between the cluster sizes at the free energy maximum and minimum, as is expected from the classical form of the ion-induced nucleation rate. However, the results show that applying the nucleation theorem to neutral systems with stable pre-nucleation clusters may lead to erroneous interpretations about the nature of the critical cluster. 相似文献
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Qing Shen Zhi-Xin Wang Jian-Feng Hu Qing-Feng Gu 《Colloids and surfaces. A, Physicochemical and engineering aspects》2004,240(1-3):107-110
In addition to recently Luner and Oh used method for characterizing of the surface free energy for cellulose ether films, this paper shows the same values however using the column wicking technique. Since re-characterized values are found larger than that Luner and Oh reported, it is suggested that the values reported by Luner and Oh may represent only for degraded samples with respect to the preparation process these authors used. In this paper, the surface free energy for cellulose ethers has been found mainly contributed by the Lifshitz–van der Waals component, e.g. of about 99%, than that of the cellulose, usually small than 97%. Whereas the Lewis acid and Lewis base components for cellulose ethers have been found decreased for the former and increased for the latter, respectively, comparing to cellulose. Additionally, it is also found that the surface free energy fro cellulose ethers seems to be decreased with the increase of the viscosity, but it seems to be greater than that of cellulose as the same as Luner and Oh found. 相似文献
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Abstract— This paper reports the present conclusions of an extended investigation on photo-sensitization of silver bromide. A general molecular packing structure for dye aggregates on the AgBr (111) surface is proposed. This structure, along with the observed spectral absorption displacements of small aggregates, is used to elucidate the phenomena of antisensitization and supersensitization. Supersensitization is seen as a partitioning of large dye aggregates into small aggregates by a deliberately added second component or by gaps between the aggregates. This partitioning isolates antisensitizing dye in a small fraction of the aggregates and minimizes its effect. The smallest aggregates are least likely to contain an antisensitizer, and show the highest quantum efficiency for photoconductivity and photographic action. Photoconductivity measurements establish that supersensitization occurs before the electron appears in the AgBr phase.
The question of direct electron injection vs. energy transfer as mechanisms for AgBr photosensitization is examined in terms of radiationless transfer to surface Ag2 S on AgBr. The absorption of surface Ag2 S is shown to be adequate for acceptance of Förster transfer from the dye, and surface Ag2 S is known to be photographically active. However, this mechanism is inefficient, and inadequate to account for observed high efficiency infrared sensitization. Direct electron injection is seen as the more probable mechanism for efficient dye sensitization of AgBr. 相似文献
The question of direct electron injection vs. energy transfer as mechanisms for AgBr photosensitization is examined in terms of radiationless transfer to surface Ag
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STUDY ON THE SURFACE MODIFICATION OF NANO-TiO2 BY GRAFTING PMMA/PBMA AND ITS THERMAL STABILITY 总被引:1,自引:0,他引:1
The surface of nano-TiO2 was encapsulated with hydroxyl-propyl-methyl cellulose (HPMC), and then cografted with acrylates. Conditions of absorbing and grafting have been studied. Modified nano-TiO2 particles were characterized by FT-IR spectra, TEM and TG analysis. It was convinced from FT-IR studies that both methyl methacrylate (MMA) and butylmethacrylate (BMA) were co-grafted onto the surface of nano-TiO2 particles. TEM images show that the surface of nano-TiO2 particles was successfully modified by a thick layer of film-like polymer. TG results demonstrate that the decomposition temperature of HPMC-g-PMMA/PBMA, which has been grafted onto the surface of nano-TiO2, is 56.9 K higher than that of HPMC-g-PMMA/PBMA. 相似文献
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非晶PET等温结晶后,用DSC、WAXD、SAXS、密度和透射电镜等方法,考察了结晶PET在升温过程中的结构变化,进一步证实了过程中发生部分熔融再结晶;同时形态也起了明显变化:片晶增厚,片晶侧向尺寸增大,由节瘤状晶粒堆砌部分地转变为典型的片晶堆砌,构成片晶的微晶尺寸增大,晶体趋于完善,折迭表面的规则折迭增加。这样,在等温结晶时生成的结构状态转变为更稳定的形态,因而相应地在DSC曲线上出现两个熔融峰。 相似文献
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Unequal-sphere packing model is applied for the simulation of large number of hexagonal adlayer structures with surface coverage between theta=13 and theta=1 on the hexagonal substrate, with atomic radius of the adsorbate and substrate atoms as the only input. Each structure is characterized with respect to collective adlayer properties: the average adlayer height and the adlayer roughness. The distribution of hexagonal arrangements is presented in a special plot, which can be used for identification and characterization of hexagonal adlayers of different surface coverages and atomic registries. The most likely structures are related to the extreme values of our model parameters. The usefulness of this methodology is successfully demonstrated by comparison with some real adsorbate-substrate systems, i.e., halogens and rare gases adsorbed on (111) surface. Besides the agreement with experimental results, our model offers new insight into the formation of atomic adlayers and detailed analysis of the atomic registry. We believe that our approach will be of use for identification of probable structures among the large number of combinatorial possibilities in theoretical studies and for better interpretation of experimental results (i.e., scanning-tunneling microscopy images of atomic adlayers). 相似文献
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Abstract— Reduction of the excited singlet state of chlorophyll a , chlorophyll b , and pheophytin a at the surface of perylene, anthracene, and chrysene single crystals has been measured as hole injection current. The dependence of the quantum yield on the standard free-energy difference of the reaction was in accordance with theoretical expectations without correcting for an interaction energy. The maximum quantum yield of only about 10−2 holes per absorbed photon is ascribed to a very small effective lifetime of the excited singlet state due to concentration quenching of the excited singlet state in the adsorbed dye layer. 相似文献