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Surfaces and molecules

For a polar surface and molecules with permanent dipole moments, attraction is strong, as for water adsorption on a hydrophilic adsorbent. Similarly, for a polar surface, a molecule with a permanent quadrupole moment vidll be attracted more strongly than a similar molecule with a weaker moment for example, nitrogen is adsorbed more strongly than oxygen on zeolites (Sherman and Yon, gen. refs.). [Pg.1503]

Local Density F mctional Theory of Surfaces and Molecules... [Pg.49]

CIR-FTIR spectroscopy provides a direct technique for studying in situ hydrous metal oxide surfaces and molecules adsorbed on these surfaces (37). By itself, FTIR spectrometry is a well established technique which offers numerous advantages over dispersive (grating) IR spectrometry (1) improved accuracy in frequency measurements through the use of a HeNe laser (2) simultaneous frequency viewing (3) rapid, repetitive scanning which allows many spectra to be collected in a small time interval (4) miriimal thermal effects from IR beam and (5) no detection of sample IR emissions (38). [Pg.150]

A typical N2 adsorption measurement versus relative pressure over a solid that has both micropores and mesopores first involves essentially a mono-layer coverage of the surface up to point B shown in isotherm IV (lUPAC classification) in Figure 13.1. Up to and near point B the isotherm is similar to a Langmuir isotherm for which equilibrium is established between molecules adsorbing from the gas phase onto the bare surface and molecules desorbing from the adsorbed layer. The volume of adsorbed N2 that covers a monolayer volume, hence the surface area of N2 can then be determined from the slope of the linearized Langmuir plot when P/V is plotted against P ... [Pg.406]

This approach has the potential to resolve the time evolution of reactions at the surface and to capture short-lived reaction intermediates. As illustrated in Figure 3.23, a typical pump-probe approach uses surface- and molecule-specific spectroscopies. An intense femtosecond laser pulse, the pump pulse, starts a reaction of adsorbed molecules at a surface. The resulting changes in the electronic or vibrational properties of the adsorbate-substrate complex are monitored at later times by a second ultrashort probe pulse. This probe beam can exploit a wide range of spectroscopic techniques, including IR spectroscopy, SHG and infrared reflection-adsorption spectroscopy (IRAS). [Pg.93]

Hydrogen bonding is not responsible for surface tension in all substances, but it is responsible for it in many substances. The tension found on the surface of liquids and the rounding of drops of liquids are due to an uneven amount of hydrogen bonding between the molecules on the surface with molecules beneath the surface and molecules in the air. This uneven attraction creates a net force that is inward. [Pg.122]

The time elapsed between hitting the grain surface and molecule formation is of the order of seconds. The lifetime of the molecule in free space after ejection from the surface depends upon the region where it is released. In a cloud with a visual extinction of Av = 3 corresponding to a hydrogen column density of TVh = 5 x 1021 cm-2 the lifetime of a typical molecule will be in the order of 1013 sec. During this time the probability for photodissociation is unity. [Pg.72]

Title Isolatable, Water-Soluble, and Hydrolytically Stable Active Sulfones of Poly(Ethylene Glycol) and Related Polymers for Modification of Surfaces and Molecules... [Pg.665]

Polystyrene latex particles, 0.2 p, in diameter, have recently been used as immunochemical markers for sceuining electron microscopyS. (SEM). But applications of such a reagent are limited because the lydrophobic surface of the polystyrene particles makes them stick nonspeciflcally to many surfaces and molecules. The same disadvantage applies to agglutination tests. Furthermore, reliance on weak adsorption forces to hold the antibodies on the particles is not always satisfactoryifi and chemical bonding of antibodies to polystyrene particles is virtually... [Pg.236]

A strategy to develop new catalysts or to improve existing ones must encompass at least three aspects (i) an analysis of the catalyst structure and composition, (ii) an analysis of the interactions of reactants and products with the catalyst surface, and (iii) characterizations that should be performed under conditions as close as possible to those of the technological process, ideally as the catalyst is working and rates are measured simultaneously. It is difficult to meet all of these requirements in a single experiment, but the necessary information can be obtained in parallel investigations, and spectroscopy of the working catalytic surfaces and molecules adsorbed on them is thus the focus of much current research (7). [Pg.134]

Fig. 13.2. The effect of surface curvature on interaction between surface and molecule. Fig. 13.2. The effect of surface curvature on interaction between surface and molecule.
At this stage in the literature, we find that both STM and AFM can operate for fluids, which is technically impossible by electron microscope. This means that, for the first time in history, molecular dimensional analyses of surfaces and molecules situated at surfaces can be carried out in a liquid. This most important discovery in surface science instrumentation allows us to see... [Pg.653]

Anisotropic properties of surfaces and molecules are of particular interest for the development of low dimensional molecular nanostructures. In this regard the combination of PEEM and AFM enables the growth of 6P needles to be followed over a large scale range from nanometers to several tens of micrometers. 6P on Cu (110) (2 x 1) O is a well characterized system [1] both in terms of its electronic structure and crystalline structure and is found to be highly reproducible under UHV growth conditions. [Pg.149]

Wimmer E 1991 Density Functional Theory for Solids, Surface and Molecules from Energy Bemds to Molecular Bonds In Labanowski J R and J W Andzelm (Editors) Density Functional Methods in Chemistry. Berlin, Springer-Verlag, pp 7-31... [Pg.162]


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Bulk and Surface Water Molecules

Dye molecules, zeolite L channels nanocrystals, inner- and outer-surfaces

Inclusion Complexes Between Polymers and Cyclic Molecules Surface Activity

Interaction of Charged Surfaces with Ions and Molecules

Potential surfaces of Van der Waals molecules (N2)2 and

Quantitative SNIFTIRS and PM IRRAS of Organic Molecules at Electrode Surfaces

Stretching and Aligning DNA Molecules on Surfaces

Surface molecules

Thiophene-based materials on gold and silver surfaces strong molecule-substrate interactions

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