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Phase molecules

For bulk structural detemiination (see chapter B 1.9). the main teclmique used has been x-ray diffraction (XRD). Several other teclmiques are also available for more specialized applications, including electron diffraction (ED) for thin film structures and gas-phase molecules neutron diffraction (ND) and nuclear magnetic resonance (NMR) for magnetic studies (see chapter B1.12 and chapter B1.13) x-ray absorption fine structure (XAFS) for local structures in small or unstable samples and other spectroscopies to examine local structures in molecules. Electron microscopy also plays an important role, primarily tlirough unaging (see chapter B1.17). [Pg.1751]

Unfortunately, tire low resolution absorjDtion spectra characteristic of condensed phase molecules at room temperature frequently do not provide a lot of infonnation about tire physicochemical nature of intennediates. [Pg.2954]

POLYRATE can be used for computing reaction rates from either the output of electronic structure calculations or using an analytic potential energy surface. If an analytic potential energy surface is used, the user must create subroutines to evaluate the potential energy and its derivatives then relink the program. POLYRATE can be used for unimolecular gas-phase reactions, bimolecular gas-phase reactions, or the reaction of a gas-phase molecule or adsorbed molecule on a solid surface. [Pg.356]

Isolated gas phase molecules are the simplest to treat computationally. Much, if not most, chemistry takes place in the liquid or solid state, however. To treat these condensed phases, you must simulate continuous, constant density, macroscopic conditions. The usual approach is to invoke periodic boundary conditions. These simulate a large system (order of 10 molecules) as a continuous replication in all directions of a small box. Only the molecules in the single small box are simulated and the other boxes are just copies of the single box. [Pg.200]

Discotic Phases. Molecules which are disk-shaped rather than elongated also form thermotropic Hquid crystal phases. Usually these molecules have aromatic cores and six lateral substituents, although the predominance of six lateral substituents is solely historical molecules with four lateral substituents also can form Hquid crystal phases. Although the flatness of these molecules creates a steric effect promoting alignment of the normal to the disks, the fact that disordered side chains are also necessary for the formation of these phases (as is often the case for Hquid crystallinity in elongated molecules) should not be ignored. [Pg.195]

Special techniques are employed to sample for gases and particulate matter simultaneously (3). Sampling systems have been developed which permit the removal of gas-phase molecules from a moving airstream by diffusion to a coated surface and permit the passage of particulate matter... [Pg.185]

Liquid phase applications account for nearly 80% of the total use of activated carbon. Activated carbon used in liquid phase applications typically have a high fraction of pores in the macropore (>50nm) range. This is to permit the liquid phase molecules to diffuse more rapidly into the rest of the pore structure [15]. [Pg.240]

Whether AH for a projected reaction is based on bond-energy data, tabulated thermochemical data, or MO computations, there remain some fundamental problems which prevent reaching a final conclusion about a reaction s feasibility. In the first place, most reactions of interest occur in solution, and the enthalpy, entropy, and fiee energy associated with any reaction depend strongly on the solvent medium. There is only a limited amount of tabulated thermochemical data that are directly suitable for treatment of reactions in organic solvents. Thermodynamic data usually pertain to the pure compound. MO calculations usually refer to the isolated (gas phase) molecule. Estimates of solvation effects must be made in order to apply either experimental or computational data to reactions occurring in solution. [Pg.191]

The high enthalpy contribution results from its larger mass and size providing stronger interactions with the stationary phase molecules, and its increased entropy contribution arises from it being a terminal atom, thus prior to interaction with the stationary phase, it has greater freedom. [Pg.60]

Stationary Phase Molecule with Permanent Dipole... [Pg.68]

Stationary Phase Molecule with Negative Ionic Charge... [Pg.70]

However, in LC solutes are partitioned according to a more complicated balance among various attractive forces solutes interact with both mobile-phase molecules and stationary-phase molecules (or stationary-phase pendant groups), the stationary-phase interacts with mobile-phase molecules, parts of the stationary phase may interact with each other, and mobile-phase molecules interact with each other. Cavity formation in the mobile phase, overcoming the attractive forces of the mobile-phase molecules for each other, is an important consideration in LC but not in GC. Therefore, even though LC and GC share a considerable amount of basic theory, the mechanisms are very different on a molecular level. This translates into conditions that are very different on a practical level so different, in fact, that separate instruments are required in modern practice. [Pg.151]

Oxychlorides are less prolific, apart from the red-brown OsOCl4 (m.p. 32°C). This probably has a molecular structure in the solid state as the IR spectra of the solid, matrix-isolated and gas-phase molecules are very similar, and the volatility is consonant with this [30]. Syntheses include heating osmium in a stream of oxygen/chlorine ( oxychlorination ) and by ... [Pg.6]

It would be interesting to further examine the vaporization of Pu-intermetallics at higher temperatures in order to search for molecular vapor species involving Pu and the noble metals. Due to the directional nature of 5f electrons in Pu, they may not be involved in the bonding of the solid intermetallics, but could contribute to the stability of a gas phase molecule. Additional measurements of the thermodynamic stabilities of Np- and Am-noble metal intermetallics corresponding to the Pu phases considered in this work would also assist in establishing bonding trends. [Pg.109]

The process we have followed Is Identical with the one we used previously for the uranium/oxygen (U/0) system (1-2) and Is summarized by the procedure that Is shown In Figure 1. Thermodynamic functions for the gas-phase molecules were obtained previously (3) from experimental spectroscopic data and estimates of molecular parameters. The functions for the condensed phase have been calculated from an assessment of the available data, Including the heat capacity as a function of temperature (4). The oxygen potential Is found from extension Into the liquid phase of a model that was derived for the solid phase. Thus, we have all the Information needed to apply the procedure outlined In Figure 1. [Pg.128]

Because a chemical bond is only about 10 10 m long, special techniques have to be used to measure its length. There are two principal techniques one for solids and the other for gases. The technique used for solids, x-ray diffraction, is described in Major Technique 3, billowing Chapter 5. Microwave spectroscopy, discussed here, is used to determine bond lengths in gas-phase molecules. This branch of spectroscopy makes use of the ability of rotating molecules to absorb microwave radiation, which has a wavelength close to 1 cm. [Pg.208]

This important result is used to find the root mean square speeds of the gas-phase molecules at any temperature (Fig. 4.25). We can rewrite this equation to emphasize that, for a gas, the temperature is a measure of mean molecular speed. From... [Pg.285]

Doubling the separation of polar molecules reduces the strength of the interaction by a factor of 26 = 64, and so dipole-dipole interactions between rotating molecules have a significant effect only when the molecules are very close. We can now start to understand why the kinetic model accounts for the properties of gases so well gas molecules rotate and are far apart for most of the time, so any intermole-cular interactions between them are very weak. Equation 4 also describes attractions between rotating molecules in a liquid. However, in the liquid phase, molecules are closer than in the gas phase and therefore the dipole-dipole interactions are much stronger. [Pg.302]

The liquid phase of matter is the most difficult to visualize. We have seen that a gas-phase molecule moves with almost complete freedom. The intermolecular forces from other molecules are minimal, and movement is highly disordered. In the solid phase, a molecule is locked in place by intermolecular forces and can only oscillate around an average location. The liquid phase lies between the extremes of the gas and solid phases. The molecules are mobile, blit they cannot escape from one another completely. [Pg.308]

In the liquid phase, molecules have short-range order but not long-range... [Pg.308]

SOLUTION Reaction will take place in the direction that reduces the increase in pressure. (a) In the forward reaction, two N02 molecules combine to form one N204 molecule. Hence, compression favors the formation of N204. (b) Because neither direction corresponds to a reduction of gas-phase molecules, compressing the mixture should have no effect on the composition of the equilibrium mixture. (In practice, there will be a small effect due to the nonideality of the gases.)... [Pg.502]

Compression of a reaction mixture at equilibrium tends to drive the reaction in the direction that reduces the number of gas-phase molecules increasing the pressure by introducing an inert gas has no effect on the equilibrium composition. [Pg.502]

The lower isotherm represents the overload condition that can occur in liquid/liquid or gas/liquid systems under somewhat unique circumstances. If the interactions between solute molecules with themselves is stronger than the interactions between the solute molecules and the stationary phase molecules, then, as the concentration of solute molecules increases, the distribution coefficient of the solute with respect to the stationary phase also increases. This is because the solute molecules interact more strongly with a solution of themselves in the stationary phase than the stationary phase alone. Thus, the higher concentrations of solute in the chromatographic... [Pg.113]

A reaction mechanism is a series of simple molecular processes, such as the Zeldovich mechanism, that lead to the formation of the product. As with the empirical rate law, the reaction mechanism must be determined experimentally. The process of assembling individual molecular steps to describe complex reactions has probably enjoyed its greatest success for gas phase reactions in the atmosphere. In the condensed phase, molecules spend a substantial fraction of the time in association with other molecules and it has proved difficult to characterize these associations. Once the mecharrism is known, however, the rate law can be determined directly from the chemical equations for the individual molecular steps. Several examples are given below. [Pg.97]

Since plane waves are delocalised and of infinite spatial extent, it is natural to perform these calculations in a periodic environment and periodic boundary conditions can be used to enforce this periodicity. Periodic boundary conditions for an isolated molecule are shown schematically in Fig. 8. The molecular problem then becomes formally equivalent to an electronic structure calculation for a periodic solid consisting of one molecule per unit cell. In the limit of large separation between molecules, the molecular electronic structure of the isolated gas phase molecule is obtained accurately. [Pg.23]

Equation (10.12) is the simplest—and most generally useful—model that reflects heterogeneous catalysis. The active sites S are fixed in number, and the gas-phase molecules of component A compete for them. When the gas-phase concentration of component A is low, the k a term in Equation (10.12) is small, and the reaction is first order in a. When a is large, all the active sites are occupied, and the reaction rate reaches a saturation value of kjkd-The constant in the denominator, is formed from ratios of rate constants. This makes it less sensitive to temperature than k, which is a normal rate constant. [Pg.356]

In this figure, the activation energies of N2 dissociation are compared for the different reaction centers the (111) surface structure ofan fee crystal and a stepped surface. Activation energies with respect to the energy of the gas-phase molecule are related to the adsorption energies of the N atoms. As often found for bond activating surface reactions, a value of a close to 1 is obtained. It implies that the electronic interactions between the surface and the reactant in the transition state and product state are similar. The bond strength of the chemical bond... [Pg.6]

The chemical species present are the hypothetical gas-phase molecules, AB2, A, and AB. [Pg.1166]

Many readers will have some familiarity with the standard expressions for the angular distribution of photofragments ejected from a randomly oriented (gas-phase) molecule by perfectly polarized light ... [Pg.270]

In comparison with the case of a gas phase molecule that reacts in a monomole-cular reaction on a solid catalyst, the reciprocal of the Michaelis constant takes the place of the equilibrium constant of adsorption in the Langmuir-Hinshelwood equations. [Pg.75]

If we move the chemisorbed molecule closer to the surface, it will feel a strong repulsion and the energy rises. However, if the molecule can respond by changing its electron structure in the interaction with the surface, it may dissociate into two chemisorbed atoms. Again the potential is much more complicated than drawn in Fig. 6.34, since it depends very much on the orientation of the molecule with respect to the atoms in the surface. For a diatomic molecule, we expect the molecule in the transition state for dissociation to bind parallel to the surface. The barriers between the physisorption, associative and dissociative chemisorption are activation barriers for the reaction from gas phase molecule to dissociated atoms and all subsequent reactions. It is important to be able to determine and predict the behavior of these barriers since they have a key impact on if and how and at what rate the reaction proceeds. [Pg.255]


See other pages where Phase molecules is mentioned: [Pg.686]    [Pg.921]    [Pg.1243]    [Pg.1947]    [Pg.2996]    [Pg.237]    [Pg.448]    [Pg.451]    [Pg.59]    [Pg.62]    [Pg.83]    [Pg.37]    [Pg.38]    [Pg.356]    [Pg.102]    [Pg.457]    [Pg.521]    [Pg.229]    [Pg.56]    [Pg.242]   
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Averages Involving Functions in the Phase Space of One Molecule Only

Averages Involving Functions in the Phase Space of Two Molecules Only

Bent-core molecules different phases

Bond Lengths and Angles in Gas-Phase Molecules

Bond lengths gas-phase molecules

Chiral molecules, nematic phases

Chiral phases small molecule

Diatomic molecules phase diagram

Doped molecules, induced phase transition

Energies of Gas-Phase Molecules

Formation of Diatomic Molecules and Radicals in the Gas Phase

Hydrogen molecules phase-change rule

Interatomic distances gas-phase molecules

Ionization Energies of Gas-Phase Molecules

Jahn-Teller molecule, geometrical phase

Large molecules in the gas phase

Molecular recognition involving small gas-phase molecules

Molecule Reactions in the Gas Phase

Molecules in the gas phase

Molecules phase changes

Organic phases molecule

Orientational phase transitions in planar systems of nonpolar molecules

Phase of small molecules

Phase small-molecule emulsifiers

Phase target molecule synthesis

Phase transfer using amphiphilic molecules

Phase transitions diatomic molecules

Phase with macro molecules

Phase with small molecules

Phases discotic molecules

Rigid Nonspherical Particles or Molecules The Nematic Phase

Small Organic Molecules on Solid Phase Target Selection and Solution Studies

Small-molecule compounds solid-phase organic synthesis

Smectic A phases of strongly polar molecules

Smectic phase molecules forming

Solid-Phase Synthesis Oligomeric Molecules

Solid-Phase Synthesis Small Organic Molecules

Solid-phase molecules

Solution-phase small-molecule

Solution-phase small-molecule detection

Stationary phases small molecule

Structure gas-phase molecules

WATER MOLECULES MOVE FREELY BETWEEN THE LIQUID AND GASEOUS PHASES

Water molecules phase diagram

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