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Interactions of molecules

Onsager L 1939 Electrostatic interaction of molecules J. Phys. Chem. 43 189... [Pg.555]

The scope of this section restricts the discussion. One omitted topic is the collision and interaction of molecules with surfaces (see [20, 21] and section A3.9). This topic coimects quantum molecular dynamics in gas and condensed phases. Depending on the time scales of the interaction of a molecule witli a surface, the... [Pg.2291]

As it stands, the picture of dynamics from Eq. (29) is derived from the interaction of molecules with a continuous light source, that is, the system is at equilibrium with the oscillating light field. It is also valid if the light source is an infinitely short laser pulse, as here all frequencies are instantaneously excited. [Pg.269]

The Universal Force Field, UFF, is one of the so-called whole periodic table force fields. It was developed by A. Rappe, W Goddard III, and others. It is a set of simple functional forms and parameters used to model the structure, movement, and interaction of molecules containing any combination of elements in the periodic table. The parameters are defined empirically or by combining atomic parameters based on certain rules. Force constants and geometry parameters depend on hybridization considerations rather than individual values for every combination of atoms in a bond, angle, or dihedral. The equilibrium bond lengths were derived from a combination of atomic radii. The parameters [22, 23], including metal ions [24], were published in several papers. [Pg.350]

Some physical problems, such as those involving interaction of molecules, are usually formulated as integral equations. Monte Carlo methods are especially well-suited to their solution. This section cannot give a comprehensive treatment of such methods, but their use in... [Pg.478]

The collision diameter is at the value of s(r) equal to zero, and die maximum interaction of the molecules is where s(r) is a minimum. The interaction of molecules is thus a balance between a rapidly-varying repulsive interaction at small internuclear distances, and a more slowly varying attractive interaction as a function of r (Figure 3.7). [Pg.114]

Infrared, ultraviolet, and nuclear magnetic resonance spectroscopies differ from mass spectrometry in that they are nondestructive and involve the interaction of molecules with electromagnetic energy rather than with an ionizing source. Before beginning a study of these techniques, however, let s briefly review the nature of radiant energy and the electromagnetic spectrum. [Pg.418]

Cooperativity, the interaction of molecules on a protein resulting from the mutual binding of those molecules. The cooperativity may be positive (whereby the binding of one of the substances facilitates the interaction of the protein with the other molecule) or negative (binding of one molecule decreases the interaction of the protein with the other molecule). [Pg.278]

Coupling, processes that cause the interaction of molecules with membrane receptors to produce an observable cellular response see Chapter 2.2. [Pg.278]

Hyperbola (hyperbolic), a set of functions defining nonlinear relationships between abscissae and ordinates. This term is used loosely to describe nonlinear relationships between the initial interaction of molecules and receptors and the observed response (i.e., stimulus-response cascades of cells). [Pg.279]

The parameters obtained here from measurements of B12 and Dn over wide ranges of temperature are probably as reliable as any that have been proposed for the interaction of molecules of different species. Unfortunately they do not provide an adequate test of Eqs. 9 and 10, since each of the systems has as one of its components either helium or hydrogen (for which there are significant quantum corrections) or carbon dioxide (which does... [Pg.112]

In bulk diffusion, the predominant interaction of molecules is with other molecules in the fluid phase. This is the ordinary kind of diffusion, and the corresponding diffusivity is denoted as a- At low gas densities in small-diameter pores, the mean free path of molecules may become comparable to the pore diameter. Then, the predominant interaction is with the walls of the pore, and diffusion within a pore is governed by the Knudsen diffusivity, K-This diffusivity is predicted by the kinetic theory of gases to be... [Pg.365]

The interactions of molecules and light in the ozone layer result in a delicate balance that holds ozone concentration at a relatively constant value. Three reactions maintain this balance ... [Pg.483]

Related UHV Studies The interaction of molecules relevant for the present purpose, such as H2, O2, and H2O, with Ru(OOOl) surfaces under UHV conditions has been studied in much detail over the last decades [Diemant et al., 2003 Liu... [Pg.469]

Energy parameter characterizing the interaction of Molecule i with Molecule j (kJ kmoU1)... [Pg.711]

Noise can be also introduced by biochemical heterogeneity of the specimen. This can be a major cause of uncertainty in biological imaging. The high (three-dimensional) spatial resolution of fluorescence microscopy results in low numbers of fluorophores in the detection volume. In a typical biological sample, the number of fluorophores in the detection volume can be as low as 2-3 fluorophores for a confocal microscope equipped with a high NA objective at a fluorescent dye concentration of 100 nM. This introduces another source of noise for imaging applications, chemical or molecular noise, related to the inherent randomness of diffusion and the interaction of molecules. [Pg.126]

Gas adsorption (physisorption) is one of the most frequently used characterization methods for micro- and mesoporous materials. It provides information on the pore volume, the specific surface area, the pore size distribution, and heat of adsorption of a given material. The basic principle of the methods is simple interaction of molecules in a gas phase (adsorptive) with the surface of a sohd phase (adsorbent). Owing to van der Waals (London) forces, a film of adsorbed molecules (adsorbate) forms on the surface of the solid upon incremental increase of the partial pressure of the gas. The amount of gas molecules that are adsorbed by the solid is detected. This allows the analysis of surface and pore properties. Knowing the space occupied by one adsorbed molecule, Ag, and the number of gas molecules in the adsorbed layer next to the surface of the solid, (monolayer capacity of a given mass of adsorbent) allows for the calculation of the specific surface area, As, of the solid by simply multiplying the number of the adsorbed molecules per weight unit of solid with the space required by one gas molecule ... [Pg.128]

G. W. Ford and W. H. Weber, Electromagnetic interactions of molecules with metal surfaces, Phys. Rep. 113, 195-287 (1984). [Pg.337]

D. A. Britz, A. N. Khlobystov, Nanocovalent interactions of molecules with single walled carbon nanotubes, Chemical Society Reviews, vol. 35, pp. 637-659, 2006. [Pg.113]

The orientation of molecules at the interface depends on an interaction with both the surface and the molecules in the liquid phase, and also on the interaction within the adsorbed layer. The interaction of molecules with the electrode is stronger the weaker their interaction with other molecules in the bulk. The correlation between and 0 is linear but different for the transition metals and the sp metals. Owing to the tendency to form chemisorption bonds, transition metals bind water molecules more strongly than the sp metals. [Pg.18]

Oxide-supported metals play an important role in a wide variety of industrial chemical processes such as the catalytic treatment of automotive exhaust. The ability to exercise greater control over the interactions of molecules on metal surfaces will create new possibilities for pollution control and the provision of novel power sources. Furthermore, a deeper understanding of molecule surface interactions will present numerous opportunities for the design of nanocatalysts. [Pg.15]

The involvement of specific attractive interactions of molecules with the electrode surface (adsorption) makes the electrode process even more complex. The intensity of such interactions ranges from weak (physisorption) to strong (chemical bonds formed between adsorbate and electrode). [Pg.6]

Note A pronounced anisotropy in the shapes and interactions of molecules, or molecular aggregates is necessary for the formation of liquid crystals. [Pg.94]


See other pages where Interactions of molecules is mentioned: [Pg.2292]    [Pg.237]    [Pg.57]    [Pg.402]    [Pg.96]    [Pg.173]    [Pg.24]    [Pg.149]    [Pg.249]    [Pg.62]    [Pg.387]    [Pg.32]    [Pg.430]    [Pg.366]    [Pg.192]    [Pg.325]    [Pg.6]    [Pg.29]    [Pg.46]    [Pg.313]    [Pg.231]    [Pg.350]    [Pg.12]    [Pg.43]   
See also in sourсe #XX -- [ Pg.146 , Pg.152 ]




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A system of non-interacting molecules

Comparison of Keesom, Debye and London interactions in polar molecules

Donor-acceptor interactions of the model water molecule

Effect of soft interaction between molecules

Global investigation of small molecule interactions with proteins that constitute the cell (proteome)

Interaction energy of molecules

Interaction of Charged Surfaces with Ions and Molecules

Interaction of Electromagnetic Radiation with Molecules

Interaction of Molecules with Electromagnetic Fields Higher Order Terms

Interaction of Protein with small molecules

Interaction of two singlet carbene molecules

Interactions of NAs with Small Molecules

Molecule interaction

Noncovalent Interactions That Determine the Structure of a Protein Molecule in Water

Specific interaction sites of sugar molecules

Stationary States of Systems with Interacting Molecules

Systems of non-interacting molecules

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